CN104637966A - Semiconductor device and method of manufacturing same - Google Patents
Semiconductor device and method of manufacturing same Download PDFInfo
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Abstract
本发明涉及半导体器件及其制造方法。提供一种具有高灵敏度,产生较少模糊现象并能提供高可靠性图像的光电转换元件的半导体器件。半导体器件具有半导体衬底,第一p型外延层,第二p型外延层以及第一光电转换元件。第一p型外延层形成在半导体衬底的主表面上。第二p型外延层形成为覆盖第一p型外延层的上表面。第一光电转换元件形成在第二p型外延层中。第一和第二p型外延层每个都由硅制成,并且第一p型外延层具有高于第二p型外延层的p型杂质浓度。
The present invention relates to a semiconductor device and a method of manufacturing the same. To provide a semiconductor device of a photoelectric conversion element having high sensitivity, producing less blurring phenomenon, and providing highly reliable images. A semiconductor device has a semiconductor substrate, a first p-type epitaxial layer, a second p-type epitaxial layer, and a first photoelectric conversion element. A first p-type epitaxial layer is formed on the main surface of the semiconductor substrate. The second p-type epitaxial layer is formed to cover the upper surface of the first p-type epitaxial layer. The first photoelectric conversion element is formed in the second p-type epitaxial layer. The first and second p-type epitaxial layers are each made of silicon, and the first p-type epitaxial layer has a higher p-type impurity concentration than the second p-type epitaxial layer.
Description
相关申请交叉引用Related Application Cross Reference
将2013年11月8日提交的日本专利申请No.2013-232371的公开内容,包括说明书、附图和摘要,整体并入本文作为参考。The disclosure of Japanese Patent Application No. 2013-232371 filed on Nov. 8, 2013 including specification, drawings and abstract is hereby incorporated by reference in its entirety.
技术领域technical field
本发明涉及一种半导体器件以及制造该器件的方法,特别地,涉及一种具有光电转换元件的半导体器件以及制造该器件的方法。The present invention relates to a semiconductor device and a method of manufacturing the device, and in particular, to a semiconductor device having a photoelectric conversion element and a method of manufacturing the device.
背景技术Background technique
诸如CCD(电荷耦合器件)图像传感器以及CMOS(互补金属氧化物半导体)图像传感器的半导体成像装置需要具有高S/N比以便提供高图像质量。这意味着S(信号)的提高需要高饱和信号水平以及对光信号的高灵敏度,而N(噪声)的降低需要低暗电流值。Semiconductor imaging devices such as CCD (Charge Coupled Device) image sensors and CMOS (Complementary Metal Oxide Semiconductor) image sensors need to have a high S/N ratio in order to provide high image quality. This means that an increase in S (signal) requires a high saturation signal level and high sensitivity to optical signals, while a reduction in N (noise) requires a low dark current value.
在上述半导体成像器件中,光电转换元件中通过入射光的光电转换而获得的收集电子效率的提高需要增强对输入信号的灵敏度。特别地,长波长区域中的光信号仍然可能穿透像素区且难以致使光电转换,这会劣化光电转换元件对于收集光的效率。In the above-mentioned semiconductor imaging device, improvement in the efficiency of collecting electrons obtained by photoelectric conversion of incident light in the photoelectric conversion element requires enhancement of sensitivity to input signals. In particular, optical signals in the long wavelength region may still penetrate the pixel region and cause photoelectric conversion with difficulty, which degrades the efficiency of the photoelectric conversion element for collecting light.
此外,当提供至一个光电转换元件并在像素区深度穿透的光在其例如到达半导体成像器件的衬底时被光电转换时,例如存在光电转换电子通过衬底泄漏进相邻于该一个光电转换元件的另一光电转换元件中的可能性。而且当输入超过饱和信号水平的光信号水平时,存在电子泄漏进相邻于被输入该光信号的该一个光电转换元件的另一光电转换元件的可能。这种电子的泄漏,即所谓的模糊现象,即使有的话也会劣化该一个光电转换元件的电子检测灵敏度,并且对于检测过剩电子来说,检测信号的噪声增大会导致S/N比的下降。In addition, when light supplied to one photoelectric conversion element and penetrating at the depth of the pixel region is photoelectrically converted when it reaches, for example, the substrate of the semiconductor imaging device, for example, there is leakage of photoelectrically converted electrons through the substrate into adjacent photoelectric cells adjacent to the one photoelectric conversion element. Possibilities in another photoelectric conversion element of the conversion element. Also when an optical signal level exceeding the saturation signal level is input, there is a possibility that electrons leak into another photoelectric conversion element adjacent to the one photoelectric conversion element to which the optical signal is input. Such leakage of electrons, so-called blurring, degrades, if any, the electron detection sensitivity of the one photoelectric conversion element, and for detection of excess electrons, an increase in the noise of the detection signal leads to a decrease in the S/N ratio .
用于抑制这种现象的技术例如公开于日本未审专利申请公布No.2008-91781(专利文献1),日本未审专利申请公布No.2007-13177(专利文献2)以及日本未审专利申请公布No.2008-98601(专利文献3)中。Techniques for suppressing this phenomenon are disclosed in, for example, Japanese Unexamined Patent Application Publication No. 2008-91781 (Patent Document 1), Japanese Unexamined Patent Application Publication No. 2007-13177 (Patent Document 2), and Japanese Unexamined Patent Application Publication No. In Publication No. 2008-98601 (Patent Document 3).
[专利文献][Patent Document]
[专利文献1]日本未审专利申请公布No.2008-91781[Patent Document 1] Japanese Unexamined Patent Application Publication No. 2008-91781
[专利文献2]日本未审专利申请公布No.2007-13177[Patent Document 2] Japanese Unexamined Patent Application Publication No. 2007-13177
[专利文献3]日本未审专利申请公布No.2008-98601[Patent Document 3] Japanese Unexamined Patent Application Publication No. 2008-98601
发明内容Contents of the invention
可以通过增大在其中希望发生用于提供可由光电转换元件收集的电子的光电转换的区域深度来提高光电转换效率。在上述各个专利文献中,通过形成上述区域作为外延层,与通过离子注入技术形成相比,可以增大该区域的深度。以这种方式,可以增加希望发生光电转换的区域的深度。但是上述各个文献具有如下问题。Photoelectric conversion efficiency can be improved by increasing the depth of a region in which photoelectric conversion for supplying electrons collectable by the photoelectric conversion element is desired to occur. In each of the above-mentioned patent documents, by forming the above-mentioned region as an epitaxial layer, the depth of the region can be increased compared with formation by ion implantation technology. In this way, the depth of the region where photoelectric conversion is desired to occur can be increased. However, each of the above-mentioned documents has the following problems.
在专利文献1中,形成在p型半导体衬底上的n型半导体层具有光电转换部。在这种情况下,n型半导体层中作为少数载流子的空穴移动至光电转换部,但是空穴的迁移率小于电子的迁移率并且在移动期间发生复合的概率高。因此会降低光电转换部的电信号的灵敏度。In Patent Document 1, an n-type semiconductor layer formed on a p-type semiconductor substrate has a photoelectric conversion portion. In this case, holes as minority carriers in the n-type semiconductor layer move to the photoelectric conversion portion, but the mobility of the holes is smaller than that of electrons and the probability of recombination during movement is high. Therefore, the sensitivity of the electric signal of the photoelectric conversion part will be reduced.
在专利文献2中,硅衬底在其上具有硅锗外延层。由不同于衬底的材料制成的薄膜的形成会加速它们之间界面处的生成和复合,产生泄漏电流并劣化CMOS图像传感器的S/N比。In Patent Document 2, a silicon substrate has a silicon germanium epitaxial layer thereon. Formation of a thin film made of a material different from that of the substrate accelerates growth and recombination at the interface between them, generates leakage current, and degrades the S/N ratio of the CMOS image sensor.
在专利文献3中,仅单一p型外延层形成在衬底上。在这种情况下,外延层深度的增大会改善从红色滤光器入射进入外延层中的光的转换比,但是存在不能克服另一问题,例如模糊现象抑制效果的劣化的可能性。In Patent Document 3, only a single p-type epitaxial layer is formed on a substrate. In this case, an increase in the depth of the epitaxial layer improves the conversion ratio of light incident from the red filter into the epitaxial layer, but there is a possibility that another problem such as deterioration of blur suppression effect cannot be overcome.
将从本文说明书和附图使得本发明的另外的问题和新颖的特征显而易见。Additional problems and novel features of the present invention will be apparent from the description and drawings herein.
根据本发明一个实施例的半导体器件具有:半导体衬底,第一p型外延层,第二p型外延层以及第一光电转换元件。半导体衬底在其主表面上具有第一p型外延层。第二p型外延层覆盖第一p型外延层。第二p型外延层内具有第一光电转换元件。第一和第二p型外延层每个都由硅制成并且第一p型外延层具有高于第二p型外延层的p型杂质浓度。A semiconductor device according to one embodiment of the present invention has: a semiconductor substrate, a first p-type epitaxial layer, a second p-type epitaxial layer, and a first photoelectric conversion element. The semiconductor substrate has a first p-type epitaxial layer on its main surface. The second p-type epitaxial layer covers the first p-type epitaxial layer. There is a first photoelectric conversion element in the second p-type epitaxial layer. The first and second p-type epitaxial layers are each made of silicon and the first p-type epitaxial layer has a higher p-type impurity concentration than the second p-type epitaxial layer.
根据另一实施例的半导体器件具有:半导体衬底,掩埋杂质层,p型外延层以及第一光电转换元件。半导体衬底在其中具有掩埋杂质层。掩埋杂质层在其上具有p型外延层。p型外延层在其中具有第一光电转换元件。掩埋杂质层和p型外延层每个都由硅制成并且掩埋杂质层具有高于p型外延层的p型杂质浓度。A semiconductor device according to another embodiment has: a semiconductor substrate, a buried impurity layer, a p-type epitaxial layer, and a first photoelectric conversion element. A semiconductor substrate has a buried impurity layer therein. The buried impurity layer has a p-type epitaxial layer thereon. The p-type epitaxial layer has the first photoelectric conversion element therein. The buried impurity layer and the p-type epitaxial layer are each made of silicon and the buried impurity layer has a higher p-type impurity concentration than the p-type epitaxial layer.
根据一个实施例的制造半导体器件的方法包括如下步骤:提供具有主表面的半导体衬底,在主表面上形成第一p型外延层,形成第二p型外延层以便覆盖第一p型外延层的上表面,以及在第二p型外延层中形成第一光电转换元件。第一和第二p型外延层每个都由硅制成并且第一p型外延层具有高于第二p型外延层的p型杂质浓度。A method of manufacturing a semiconductor device according to one embodiment includes the steps of: providing a semiconductor substrate having a main surface, forming a first p-type epitaxial layer on the main surface, forming a second p-type epitaxial layer so as to cover the first p-type epitaxial layer The upper surface of the upper surface, and the first photoelectric conversion element is formed in the second p-type epitaxial layer. The first and second p-type epitaxial layers are each made of silicon and the first p-type epitaxial layer has a higher p-type impurity concentration than the second p-type epitaxial layer.
根据本发明的一个实施例,第二p型外延层能使光电转换元件检测已经通过更深区域中的光电转换而获得的电子,从而以高灵敏度驱动第一光电转换元件,并且同时,第一p型外延层用作减小模糊现象的阻挡层。这致使S/N比的改善并且由此获得具有提高了可靠性的图像。According to one embodiment of the present invention, the second p-type epitaxial layer enables the photoelectric conversion element to detect electrons that have been obtained through photoelectric conversion in a deeper region, thereby driving the first photoelectric conversion element with high sensitivity, and at the same time, the first p The epitaxial layer is used as a barrier layer to reduce blurring. This leads to an improvement of the S/N ratio and thereby obtains an image with improved reliability.
虽然在本发明的该另一实施例中,该一个实施例的第一p型外延层由掩埋杂质层替代,并且该一个实施例的第二p型外延层由p型外延层替代,但是该另一实施例基本上具有类似于该一个实施例的优点。Although in this other embodiment of the present invention, the first p-type epitaxial layer of this one embodiment is replaced by a buried impurity layer, and the second p-type epitaxial layer of this one embodiment is replaced by a p-type epitaxial layer, the Another embodiment basically has advantages similar to the one embodiment.
在采用根据本发明的该一个实施例的制造方法制造的半导体器件中,第二p型外延层能使光电转换元件检测通过已经发生在更深区域中的光电转换产生的电子,由此以高灵敏度驱动第一光电转换元件,并且同时,第一类型外延层用作用于减小模糊现象的阻挡层。因此,能提供具有改善了S/N比并能提供高可靠的图像的半导体器件。In the semiconductor device manufactured by the manufacturing method according to this one embodiment of the present invention, the second p-type epitaxial layer enables the photoelectric conversion element to detect electrons generated by photoelectric conversion that has occurred in a deeper region, thereby with high sensitivity The first photoelectric conversion element is driven, and at the same time, the first type epitaxial layer serves as a barrier layer for reducing the blurring phenomenon. Therefore, a semiconductor device having an improved S/N ratio and capable of providing highly reliable images can be provided.
附图说明Description of drawings
图1是示出根据一个实施例的晶片形式的半导体器件的示意平面图;1 is a schematic plan view showing a semiconductor device in the form of a wafer according to one embodiment;
图2是由图1的虚线包围的区域II的示意图;Fig. 2 is the schematic diagram of the region II enclosed by the dotted line of Fig. 1;
图3是示出图2的像素部的构造的示意平面图;3 is a schematic plan view showing the configuration of a pixel portion of FIG. 2;
图4是示出第一实施例的像素部的构造的示意截面图;4 is a schematic cross-sectional view showing the configuration of a pixel portion of the first embodiment;
图5是示出制造根据第一实施例的半导体器件的方法的第一步骤的示意截面图;5 is a schematic cross-sectional view showing a first step of the method of manufacturing the semiconductor device according to the first embodiment;
图6是示出制造根据第一实施例的半导体器件的方法的第二步骤的示意截面图;6 is a schematic cross-sectional view showing a second step of the method of manufacturing the semiconductor device according to the first embodiment;
图7是示出制造根据第一实施例的半导体器件的方法的第三步骤的示意截面图;7 is a schematic cross-sectional view showing a third step of the method of manufacturing the semiconductor device according to the first embodiment;
图8是示出制造根据第一实施例的半导体器件的方法的第四步骤的示意截面图;8 is a schematic cross-sectional view showing a fourth step of the method of manufacturing the semiconductor device according to the first embodiment;
图9是示出制造根据第一实施例的半导体器件的方法的第五步骤的示意截面图;9 is a schematic cross-sectional view showing a fifth step of the method of manufacturing the semiconductor device according to the first embodiment;
图10是示出制造根据第一实施例的半导体器件的方法的第六步骤的示意截面图;10 is a schematic sectional view showing a sixth step of the method of manufacturing the semiconductor device according to the first embodiment;
图11是示出第一实施例的比较实例中的像素部的构造的示意截面图;11 is a schematic cross-sectional view showing the configuration of a pixel portion in a comparative example of the first embodiment;
图12是通过光的波长示出发生光电转换的深度和电子收集效率之间关系的曲线图;12 is a graph showing the relationship between the depth at which photoelectric conversion occurs and electron collection efficiency by wavelength of light;
图13是示出第一实施例和比较实例中来自红光和绿光的电子的收集效率的曲线图;13 is a graph showing collection efficiencies of electrons from red light and green light in the first embodiment and a comparative example;
图14是示出第二p型外延层的膜厚和内量子效率之间关系的曲线图;14 is a graph showing the relationship between the film thickness of the second p-type epitaxial layer and the internal quantum efficiency;
图15是通过衬底中形成的缺陷的存在或不存在示出第二p型外延层的膜厚,内量子效率以及电子串扰之间关系的曲线图;15 is a graph showing the relationship between the film thickness of the second p-type epitaxial layer, internal quantum efficiency and electron crosstalk by the presence or absence of defects formed in the substrate;
图16是示出第二实施例中的像素部的构造的示意截面图;16 is a schematic cross-sectional view showing the configuration of a pixel portion in the second embodiment;
图17是示出制造根据第二实施例的半导体器件的方法的第一步骤的示意截面图;17 is a schematic cross-sectional view showing a first step of a method of manufacturing a semiconductor device according to a second embodiment;
图18是示出制造根据第二实施例的半导体器件的方法的第二步骤的示意截面图;18 is a schematic cross-sectional view showing a second step of the method of manufacturing the semiconductor device according to the second embodiment;
图19是示出制造根据第二实施例的半导体器件的方法的第三步骤的示意截面图;19 is a schematic cross-sectional view showing a third step of the method of manufacturing the semiconductor device according to the second embodiment;
图20是示出制造根据第二实施例的半导体器件的方法的第四步骤的示意截面图;20 is a schematic cross-sectional view showing a fourth step of the method of manufacturing the semiconductor device according to the second embodiment;
图21是示出制造根据第二实施例的半导体器件的方法的第五步骤的示意截面图;21 is a schematic cross-sectional view showing a fifth step of the method of manufacturing the semiconductor device according to the second embodiment;
图22是示出第三实施例的像素部的构造的示意截面图;22 is a schematic cross-sectional view showing the configuration of a pixel portion of the third embodiment;
图23是示出制造根据第三实施例的半导体器件的方法的第一步骤的示意截面图;23 is a schematic sectional view showing a first step of a method of manufacturing a semiconductor device according to a third embodiment;
图24是示出制造根据第三实施例的半导体器件的方法的第二步骤的示意截面图;24 is a schematic sectional view showing a second step of the method of manufacturing the semiconductor device according to the third embodiment;
图25是示出制造根据第三实施例的半导体器件的方法的第三步骤的示意截面图;25 is a schematic cross-sectional view showing a third step of the method of manufacturing the semiconductor device according to the third embodiment;
图26是示出制造根据第三实施例的半导体器件的方法的第四步骤的示意截面图;26 is a schematic sectional view showing a fourth step of the method of manufacturing the semiconductor device according to the third embodiment;
图27是示出第四实施例中的像素部的构造的示意截面图;27 is a schematic cross-sectional view showing the configuration of a pixel portion in the fourth embodiment;
图28是示出制造根据第四实施例的半导体器件的方法的第一步骤的示意截面图;28 is a schematic sectional view showing a first step of a method of manufacturing a semiconductor device according to a fourth embodiment;
图29是示出制造根据第四实施例的半导体器件的方法的第二步骤的示意截面图;29 is a schematic cross-sectional view showing a second step of the method of manufacturing the semiconductor device according to the fourth embodiment;
图30是示出第五实施例中的像素部的构造的示意截面图;30 is a schematic cross-sectional view showing the configuration of a pixel portion in the fifth embodiment;
图31是示出第六实施例中的像素部的构造的示意截面图;31 is a schematic cross-sectional view showing the configuration of a pixel portion in the sixth embodiment;
图32是示出第七实施例中的像素部的构造的示意截面图;32 is a schematic cross-sectional view showing the configuration of a pixel portion in the seventh embodiment;
图33是示出制造根据第七实施例的半导体器件的方法的一个步骤的示意截面图;33 is a schematic sectional view showing a step of a method of manufacturing a semiconductor device according to a seventh embodiment;
图34是示出第八实施例中的像素部的构造的示意截面图;34 is a schematic cross-sectional view showing the configuration of a pixel portion in the eighth embodiment;
图35是示出第九实施例中的像素部的构造的示意截面图;35 is a schematic cross-sectional view showing the configuration of a pixel portion in the ninth embodiment;
图36是示出制造根据第九实施例的半导体器件的方法的第一步骤的示意截面图;36 is a schematic sectional view showing a first step of a method of manufacturing a semiconductor device according to a ninth embodiment;
图37是示出制造根据第九实施例的半导体器件的方法的第二步骤的示意截面图;37 is a schematic cross-sectional view showing a second step of the method of manufacturing the semiconductor device according to the ninth embodiment;
图38是示出制造根据第九实施例的半导体器件的方法的第三步骤的示意截面图;38 is a schematic cross-sectional view showing a third step of the method of manufacturing the semiconductor device according to the ninth embodiment;
图39是示出第十实施例中的像素部的构造的示意截面图;39 is a schematic cross-sectional view showing the configuration of a pixel portion in the tenth embodiment;
图40是示出制造根据第十实施例的半导体器件的方法的第一步骤的示意截面图;40 is a schematic cross-sectional view showing a first step of the method of manufacturing the semiconductor device according to the tenth embodiment;
图41是示出制造根据第十实施例的半导体器件的方法的第二步骤的示意截面图;41 is a schematic sectional view showing a second step of the method of manufacturing the semiconductor device according to the tenth embodiment;
图42是示出制造根据第十实施例的半导体器件的方法的第三步骤的示意截面图;42 is a schematic cross-sectional view showing a third step of the method of manufacturing the semiconductor device according to the tenth embodiment;
图43是示出第十一实施例中的像素部的构造的示意截面图;43 is a schematic cross-sectional view showing the configuration of a pixel portion in the eleventh embodiment;
图44是示出制造根据第十一实施例的半导体器件的方法的第一步骤的示意截面图;44 is a schematic cross-sectional view showing the first step of the method of manufacturing the semiconductor device according to the eleventh embodiment;
图45是示出制造根据第十一实施例的半导体器件的方法的第二步骤的示意截面图;以及45 is a schematic sectional view showing a second step of the method of manufacturing the semiconductor device according to the eleventh embodiment; and
图46是示出根据一个实施例的半导体器件的像素部的构造要点的示意截面图。FIG. 46 is a schematic cross-sectional view showing a configuration outline of a pixel portion of a semiconductor device according to one embodiment.
具体实施方式Detailed ways
以下将根据一些附图说明一个实施例。An embodiment will be described below with reference to some drawings.
(第一实施例)(first embodiment)
首先将参考图1至3说明根据一个实施例的半导体器件的半导体衬底的主表面上的元件形成区的布置。First, an arrangement of an element formation region on a main surface of a semiconductor substrate of a semiconductor device according to an embodiment will be described with reference to FIGS. 1 to 3 .
如图1所示,半导体器件形成在具有作为基底的半导体衬底SUB的半导体晶片SCW上。半导体晶片SCW具有其中将要形成多个半导体成像器件的多个芯片区IMC。芯片区IMC每个都具有矩形平面形状且它们布置成矩阵。芯片区IMC之间具有划线区DLR。As shown in FIG. 1, a semiconductor device is formed on a semiconductor wafer SCW having a semiconductor substrate SUB as a base. The semiconductor wafer SCW has a plurality of chip regions IMC in which a plurality of semiconductor imaging devices are to be formed. The chip regions IMC each have a rectangular planar shape and they are arranged in a matrix. There is a scribe region DLR between the chip regions IMC.
如图2所示,芯片区IMC每个都具有像素部和外围电路部。像素部位于芯片区IMC中心并且外围电路部位于围绕像素部的区域中。As shown in FIG. 2, the chip regions IMC each have a pixel portion and a peripheral circuit portion. The pixel portion is located at the center of the chip region IMC and the peripheral circuit portion is located in an area surrounding the pixel portion.
如图3所示,像素部主要具有转移晶体管TMI、放大晶体管AMI以及选择晶体管SMI,并且例如由它们构成的多个所谓的固体成像器件以矩阵布置。在图3中,多个晶体管TMI布置成矩阵。虽然放大晶体管AMI和选择晶体管SMI的数量分别仅为一个,但是替代地,多个放大晶体管AMI或多个选择晶体管SMI可以被布置成矩阵。As shown in FIG. 3 , the pixel section mainly has a transfer transistor TMI, an amplification transistor AMI, and a selection transistor SMI, and for example, a plurality of so-called solid-state imaging devices constituted by them are arranged in a matrix. In FIG. 3, a plurality of transistors TMI are arranged in a matrix. Although the numbers of the amplification transistors AMI and the selection transistors SMI are only one, respectively, instead, a plurality of amplification transistors AMI or a plurality of selection transistors SMI may be arranged in a matrix.
转移晶体管TMI具有转移栅Tx,光电二极管PD以及电容区FD。转移栅Tx是用作转移晶体管TMI的栅电极的区域。光电二极管PD是用于通过光电转换将入射光转换成电信号,即,诸如电子的电荷的光电转换元件。光电二极管PD部分地是用于在其接收光时提供电荷的区域,因此当整个转移晶体管TMI被认为是MOS(金属氧化物半导体)晶体管时,光电二极管PD对应于晶体管的源极区。电容区FD对应于常规MOS晶体管的漏极区,因为其将由光电二极管PD提供的电荷转换成电信号(电压)并将它们转移给另一晶体管(例如将在下文说明的放大晶体管AMI)。因此转移晶体管TMI整体被认为是具有类似于MOS晶体管的构造的晶体管。The transfer transistor TMI has a transfer gate Tx, a photodiode PD and a capacitance region FD. The transfer gate Tx is a region serving as a gate electrode of the transfer transistor TMI. The photodiode PD is a photoelectric conversion element for converting incident light into an electrical signal, that is, charges such as electrons, by photoelectric conversion. The photodiode PD is partly a region for supplying charges when it receives light, so when the entire transfer transistor TMI is regarded as a MOS (Metal Oxide Semiconductor) transistor, the photodiode PD corresponds to a source region of the transistor. Capacitance region FD corresponds to a drain region of a conventional MOS transistor because it converts charges supplied from photodiode PD into electrical signals (voltage) and transfers them to another transistor (eg, amplification transistor AMI to be described later). The transfer transistor TMI as a whole is thus regarded as a transistor having a configuration similar to that of a MOS transistor.
放大晶体管AMI是用于放大通过光电二极管PD处的光电转换而获得的信号电荷的MOS晶体管。转移晶体管TMI是用于将光电二极管PD处的转换之后积累的信号电荷转移至放大晶体管AMI的MOS晶体管。选择晶体管SMI是用于选择布置成矩阵的像素耦接到的行选择线中的任一个并选择将要耦接至该行选择线的像素的MOS晶体管。The amplification transistor AMI is a MOS transistor for amplifying signal charges obtained by photoelectric conversion at the photodiode PD. The transfer transistor TMI is a MOS transistor for transferring signal charges accumulated after conversion at the photodiode PD to the amplification transistor AMI. The selection transistor SMI is a MOS transistor for selecting any one of row selection lines to which pixels arranged in a matrix are coupled and selecting a pixel to be coupled to the row selection line.
形成作为隔离区的沟槽隔离TI以便围绕各个晶体管TMI、AMI、SMI(包括其中将要形成放大晶体管AMI和选择晶体管SMI的有源区ACR)。A trench isolation TI as an isolation region is formed so as to surround the respective transistors TMI, AMI, SMI (including the active region ACR in which the amplification transistor AMI and the selection transistor SMI are to be formed).
参考图4,以下将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移晶体管TMI的构造。Referring to FIG. 4 , the configurations of the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described in detail below.
图4是沿图3的线IV-IV截取的部分的示意截面图。如图4所示,包括图3中所示的光电二极管PD的转移晶体管TMI形成在对应于图1的半导体衬底SUB的p型衬底PSB1的主表面SI上。p型衬底PSB1例如是由硅制成的p型衬底。FIG. 4 is a schematic cross-sectional view of a portion taken along line IV-IV of FIG. 3 . As shown in FIG. 4 , a transfer transistor TMI including the photodiode PD shown in FIG. 3 is formed on the main surface SI of the p-type substrate PSB1 corresponding to the semiconductor substrate SUB of FIG. 1 . The p-type substrate PSB1 is, for example, a p-type substrate made of silicon.
p型衬底PSB1在其主表面S1上具有通过所谓的外延生长而形成的第一p型外延层PE1。第一p型外延层PE1具有由通过所谓的外延生长而形成的第二外延层PE2覆盖的上表面。在图4中,特别是在左侧上,形成第二外延层PE2以便覆盖第一p型外延层PE1的上表面。第一外延层PE1和第二外延层PE2每个都由硅制成。第一p型外延层PE1具有高于第二p型外延层PE2的p型杂质浓度。特别是在本实施例中,第一p型外延层PE1可以具有高于p型衬底PSB1的p型杂质浓度。第二外延层PE2具有大于第一外延层PE1的厚度。The p-type substrate PSB1 has on its main surface S1 a first p-type epitaxial layer PE1 formed by so-called epitaxial growth. The first p-type epitaxial layer PE1 has an upper surface covered with a second epitaxial layer PE2 formed by so-called epitaxial growth. In FIG. 4 , particularly on the left side, the second epitaxial layer PE2 is formed so as to cover the upper surface of the first p-type epitaxial layer PE1 . Each of the first epitaxial layer PE1 and the second epitaxial layer PE2 is made of silicon. The first p-type epitaxial layer PE1 has a higher p-type impurity concentration than the second p-type epitaxial layer PE2. Especially in this embodiment, the first p-type epitaxial layer PE1 may have a p-type impurity concentration higher than that of the p-type substrate PSB1. The second epitaxial layer PE2 has a thickness greater than that of the first epitaxial layer PE1.
第二外延层PE2具有两个像素区,即沿p型衬底PSB1的主表面S1的方向布置的第一像素区RPx和第二像素区GPx。第一像素区RPx和第二像素区GPx由特别是相对接近第二p型外延层PE2的表面的浅区中的沟槽隔离TI围绕。这意味着第一像素区RPx和第二像素区GPx通过夹在其间的沟槽隔离TI而彼此电绝缘。The second epitaxial layer PE2 has two pixel regions, ie, a first pixel region RPx and a second pixel region GPx arranged along the direction of the main surface S1 of the p-type substrate PSB1. The first pixel region RPx and the second pixel region GPx are surrounded by the trench isolation TI in a shallow region, especially relatively close to the surface of the second p-type epitaxial layer PE2. This means that the first pixel region RPx and the second pixel region GPx are electrically insulated from each other by the trench isolation TI sandwiched therebetween.
第一像素区RPx和第二像素区GPx在第二p型外延层PE2的表面处(图4的上侧)分别具有转移晶体管TMI。第一像素区RPx的转移晶体管TMI主要具有光电二极管PD1(第一光电转换元件)、电容区FD、栅极绝缘膜GI以及转移栅Tx。The first pixel region RPx and the second pixel region GPx respectively have transfer transistors TMI at the surface (upper side of FIG. 4 ) of the second p-type epitaxial layer PE2. The transfer transistor TMI of the first pixel region RPx mainly has a photodiode PD1 (first photoelectric conversion element), a capacitor region FD, a gate insulating film GI, and a transfer gate Tx.
光电二极管PD1存在于形成在第二p型外延层PE2的表面中的p型区SPR的正下方。换言之,光电二极管PD1掩埋在第二p型外延层PE2中。电容区FD布置在第二外延层PE2的表面中并与光电二极管PD1间隔一定距离。转移栅Tx经由在光电二极管PD1和电容区FD之间夹着的区域中的栅极绝缘膜GI而位于第二外延层PE2的表面上。The photodiode PD1 exists right below the p-type region SPR formed in the surface of the second p-type epitaxial layer PE2. In other words, the photodiode PD1 is buried in the second p-type epitaxial layer PE2. The capacitive region FD is arranged in the surface of the second epitaxial layer PE2 at a distance from the photodiode PD1. The transfer gate Tx is located on the surface of the second epitaxial layer PE2 via the gate insulating film GI in the region sandwiched between the photodiode PD1 and the capacitance region FD.
表面p型区SPR是形成在光电二极管PD1的正上方并具有高于第二p型外延层PE2的p型杂质浓度的区域。保护环GR是形成在第二p型外延层PE2的表面上并且同时形成在光电二极管PD1的侧部上(沟槽隔离TI)并具有高于第二p型外延层PE2的p型杂质浓度的区域。这些区域SPR和GR每个都形成为抑制光电二极管PD1附近的耗尽层的扩展以及光电子的复合(消失)。The surface p-type region SPR is a region formed right above the photodiode PD1 and having a higher p-type impurity concentration than the second p-type epitaxial layer PE2. The guard ring GR is formed on the surface of the second p-type epitaxial layer PE2 and at the same time on the side of the photodiode PD1 (trench isolation TI) and has a p-type impurity concentration higher than that of the second p-type epitaxial layer PE2. area. Each of these regions SPR and GR is formed to suppress the expansion of the depletion layer near the photodiode PD1 and the recombination (disappearance) of photoelectrons.
第二像素区GPx的转移晶体管TM1具有基本上类似于第一像素区RPx的转移晶体管TMI的构造,除形成光电二极管PD2(第二光电转换元件)以代替构成转移晶体管TMI的光电二极管PD1之外。类似于光电二极管PD1,光电二极管PD2因此掩埋在第二p型外延层PE2中。The transfer transistor TM1 of the second pixel region GPx has a configuration substantially similar to that of the transfer transistor TMI of the first pixel region RPx, except that a photodiode PD2 (second photoelectric conversion element) is formed instead of the photodiode PD1 constituting the transfer transistor TMI. . Like the photodiode PD1, the photodiode PD2 is thus buried in the second p-type epitaxial layer PE2.
光电二极管PD1和PD2,以及电容区FD每个都形成为第二p型外延层PE2中的n型杂质区,并且它们分别作为n型MOS晶体管的源极区和漏极区。光电二极管PD1是具有将入射在其上的光进行光电转换的功能的器件。入射光到电子的转换(光电转换)本身无需发生在作为n型杂质区的光电二极管PD1中,并且如将在下文说明的,其可发生在诸如p型外延层PE2或p型衬底PSB1的其他区域中。但是n型杂质区具有收集由光转换的电子的作用,因此本文所用术语“光电二极管PD1”和“光电二极管PD2”定义为意指收集由光电转换形成的电子的区域。The photodiodes PD1 and PD2, and the capacitance region FD are each formed as an n-type impurity region in the second p-type epitaxial layer PE2, and they function as a source region and a drain region of an n-type MOS transistor, respectively. The photodiode PD1 is a device having a function of photoelectrically converting light incident thereon. The conversion of incident light into electrons (photoelectric conversion) itself does not need to occur in the photodiode PD1 as an n-type impurity region, and as will be described later, it may occur in a layer such as the p-type epitaxial layer PE2 or the p-type substrate PSB1. in other areas. However, the n-type impurity region has a role of collecting electrons converted by light, so the terms "photodiode PD1" and "photodiode PD2" used herein are defined to mean regions collecting electrons formed by photoelectric conversion.
在图3中,图4的光电二极管PD1和光电二极管PD2都被称为“光电二极管PD”。光电二极管PD1和光电二极管PD2在入射在其上的光的平均波长方面彼此不同。In FIG. 3 , both the photodiode PD1 and the photodiode PD2 of FIG. 4 are referred to as "photodiode PD". The photodiode PD1 and the photodiode PD2 are different from each other in the average wavelength of light incident thereon.
更具体地,光电二极管PD1具备未示出的红色滤光器,因此其通过红色滤光器将照射在光电二极管PD1的光接收为红光。类似地,光电二极管PD2例如具备未示出的绿色滤光器,因此其通过绿色滤光器将照射在光电二极管PD2的光接收为绿光。光电二极管PD2可以具备蓝色滤光器以替代绿色滤光器。More specifically, the photodiode PD1 is provided with an unillustrated red filter, so it receives the light irradiated on the photodiode PD1 as red light through the red filter. Similarly, the photodiode PD2 is equipped with, for example, an unshown green filter, so it receives the light irradiated on the photodiode PD2 as green light through the green filter. Photodiode PD2 may be provided with a blue filter instead of a green filter.
因此,光电二极管PD1可以接收的光是红光,并且其具有相对长的平均波长(可见光中最长的波长)。另一方面,光电二极管PD2接收具有短于光电二极管PD1可以接受的光的平均波长的光(绿或蓝光)。因为第一像素区RPx和第二像素区GPx在沿p型衬底PSB1的主表面S1的方向上布置,因此光电二极管PD1和光电二极管PD2在沿p型衬底PSB1的主表面SB1的方向上布置。Therefore, the light that the photodiode PD1 can receive is red light, and it has a relatively long average wavelength (the longest wavelength in visible light). On the other hand, photodiode PD2 receives light (green or blue light) having an average wavelength shorter than that of light that photodiode PD1 can accept. Because the first pixel region RPx and the second pixel region GPx are arranged in the direction along the main surface S1 of the p-type substrate PSB1, the photodiode PD1 and the photodiode PD2 are arranged in the direction along the main surface SB1 of the p-type substrate PSB1 layout.
在第二像素区GPx中,光电二极管PD2在其下以及在第二外延层PE2中具有第一注入区PJ1(第一p型杂质区)。通过所谓的离子注入技术形成第一注入区PJ1以便覆盖上表面(因此与第一p型外延层PE1的上表面接触),并且其具有高于第二p型外延层PE2的p型杂质浓度。In the second pixel region GPx, the photodiode PD2 has a first injection region PJ1 (first p-type impurity region) thereunder and in the second epitaxial layer PE2. First implantation region PJ1 is formed by so-called ion implantation technique so as to cover the upper surface (and thus be in contact with the upper surface of first p-type epitaxial layer PE1), and has a higher p-type impurity concentration than second p-type epitaxial layer PE2.
另一方面,如上所述,包括了光电二极管PD1的第一像素区RPx以及包括了光电二极管PD2的第二像素区GPx在它们之间的边界区处具有用于将这些区域彼此电绝缘的沟槽隔离TI。第二p型外延层PE2中的沟槽隔离TI在沟槽隔离的正下方具有第二注入区PJ2(第二p型杂质区)。第二注入区PJ2通过所谓的离子注入技术形成。第二注入区PJ2具有高于第二p型外延层PE2的p型杂质浓度。On the other hand, as described above, the first pixel region RPx including the photodiode PD1 and the second pixel region GPx including the photodiode PD2 have a trench for electrically insulating these regions from each other at the boundary region therebetween. Slot isolation TI. The trench isolation TI in the second p-type epitaxial layer PE2 has a second implantation region PJ2 (second p-type impurity region) directly below the trench isolation. The second implantation region PJ2 is formed by a so-called ion implantation technique. The second implantation region PJ2 has a p-type impurity concentration higher than that of the second p-type epitaxial layer PE2.
形成在第二像素区GPx中的第一注入区PJ1优选相对于附图中的水平方向延伸至第一像素区RPx和第二像素区GPx之间的边界部。在这种情况下,形成第二注入区PJ2以便到达边界部处的第一注入区PJ1的上表面(以便在第一注入区PJ1的上表面上使第二注入区与第一注入区PJ1接触)。而且,第二注入区PJ2优选形成为在最上部与正上方的沟槽隔离TI接触。换言之,第二注入区PJ2优选形成在第一像素区RPx和第二像素区GPx之间的边界部处,以便在被夹在其间的同时将第一注入区PJ1和沟槽隔离TI彼此耦接。The first injection region PJ1 formed in the second pixel region GPx preferably extends to a boundary portion between the first pixel region RPx and the second pixel region GPx with respect to a horizontal direction in the drawing. In this case, the second implantation region PJ2 is formed so as to reach the upper surface of the first implantation region PJ1 at the boundary portion (so that the second implantation region is in contact with the first implantation region PJ1 on the upper surface of the first implantation region PJ1 ). Also, the second implantation region PJ2 is preferably formed so as to be in contact with the trench isolation TI directly above at the uppermost portion. In other words, the second injection region PJ2 is preferably formed at a boundary portion between the first pixel region RPx and the second pixel region GPx so as to couple the first injection region PJ1 and the trench isolation TI to each other while being sandwiched therebetween. .
但是优选的是第一注入区PJ1仅形成在第二像素区GPx中以及第一像素区RPx和第二像素区GPx之间的边界部处,并且不形成在第一像素区RPx中。因为第一注入区PJ1形成在第二像素区GPx中的第二p型外延层PE2中的最下侧(p型衬底PSB1的侧面上)上,因此第二像素区GPx中的第二p型外延层PE2的厚度显然小于第一像素区RPx中的第二p型外延层PE2的厚度。But it is preferable that the first injection region PJ1 is formed only in the second pixel region GPx and at a boundary portion between the first pixel region RPx and the second pixel region GPx, and is not formed in the first pixel region RPx. Since the first injection region PJ1 is formed on the lowermost side (on the side of the p-type substrate PSB1) of the second p-type epitaxial layer PE2 in the second pixel region GPx, the second p-type epitaxial layer PE2 in the second pixel region GPx The thickness of the p-type epitaxial layer PE2 is obviously smaller than the thickness of the second p-type epitaxial layer PE2 in the first pixel region RPx.
通过将第二p型外延层PE2的p型杂质浓度设定为小于第一p型外延层PE1以及第一和第二注入区PJ1和PJ2的杂质浓度,可以将内部残余的缺陷密度控制得尽可能低。另一方面,将p型衬底PSB1中的缺陷密度控制得尽可能高。因此p型衬底PSB1中残余的缺陷密度高于第二p型外延层PE2的缺陷密度。By setting the p-type impurity concentration of the second p-type epitaxial layer PE2 to be lower than the impurity concentrations of the first p-type epitaxial layer PE1 and the first and second implanted regions PJ1 and PJ2, the internal residual defect density can be controlled as much as possible. probably low. On the other hand, the defect density in the p-type substrate PSB1 is controlled as high as possible. Therefore, the residual defect density in the p-type substrate PSB1 is higher than the defect density of the second p-type epitaxial layer PE2.
p型衬底PSB1具有(多个)微小缺陷D1和扩展缺陷D2a的混合物。术语“缺陷密度”是指微小缺陷D1和扩展缺陷D2a两者的密度或仅扩展缺陷D2a的密度。The p-type substrate PSB1 has a mixture of minute defect(s) D1 and extended defect D2a. The term "defect density" refers to the density of both the minute defects D1 and the extended defects D2a or only the extended defects D2a.
控制p型衬底PSB1中的缺陷密度以便使p型衬底PSB1中作为少数载流子的电子寿命足够短于p型外延层PE2中的电子的载流子寿命,例如10ns以上但不大于500ns。Controlling the defect density in the p-type substrate PSB1 so that the lifetime of electrons serving as minority carriers in the p-type substrate PSB1 is sufficiently shorter than the carrier lifetime of electrons in the p-type epitaxial layer PE2, for example, more than 10 ns but not greater than 500 ns .
通过热处理致使p型衬底PSB1中被称为“BMD”(体微小缺陷)的微小氧化物沉淀核的生长而形成微小缺陷D1。通过热处理p型衬底PSB1同时将诸如氩或硅的杂质元素通过离子注入技术引入p型衬底PSB1中而形成扩展缺陷D2a。它们是由于由此引入的杂质元素而产生的缺陷(第二扩展缺陷)。Microdefects D1 are formed by heat treatment causing the growth of microscopic oxide precipitation nuclei called "BMD" (bulk microdefects) in the p-type substrate PSB1. The extended defect D2a is formed by heat-treating the p-type substrate PSB1 while introducing an impurity element such as argon or silicon into the p-type substrate PSB1 by an ion implantation technique. They are defects (second extended defects) due to the impurity elements thus introduced.
参考图5至10,将说明制造构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移晶体管TMI的方法。在图5至10中,示出类似于图4的区域处理。Referring to FIGS. 5 to 10 , a method of manufacturing the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described. In FIGS. 5 to 10 , area processing similar to that of FIG. 4 is shown.
如图5中所示,首先,提供是例如由硅制成的p型衬底并具有主表面S1的p型衬底PSB1。p型衬底PSB1具有p型杂质浓度,例如优选5E14cm-3以上但是不大于1E16cm-3的硼浓度。形成p型衬底PSB1以便具有等于将在下文说明的第二p型外延层PE2中的杂质浓度的p型杂质浓度。通过采用一般公知方法热处理p型衬底PSB1,p型衬底PSB1中的氧形成为微小缺陷核Dc1,微小缺陷核Dc1例如是形成BMD的核。由此形成的多个微小缺陷核Dc1分散在p型衬底PSB1中。As shown in FIG. 5 , first, a p-type substrate PSB1 that is a p-type substrate made of, for example, silicon and has a main surface S1 is provided. The p-type substrate PSB1 has a p-type impurity concentration, for example, a boron concentration of preferably 5E14 cm −3 or more but not more than 1E16 cm −3 . The p-type substrate PSB1 is formed so as to have a p-type impurity concentration equal to the impurity concentration in the second p-type epitaxial layer PE2 to be described later. By heat-treating the p-type substrate PSB1 by a generally known method, the oxygen in the p-type substrate PSB1 forms tiny defect nuclei Dc1 , such as nuclei for forming BMD. A plurality of minute defect nuclei Dc1 thus formed are dispersed in the p-type substrate PSB1.
如图6中所示,通过采用常规离子注入技术将例如硅或氩的杂质元素从p型衬底PSB1的主表面S1上方引入p型衬底PSB1。随后,通过一般公知方法再次热处理p型衬底PSB1,这样将诸如硅或氩的引入的杂质元素嵌入衬底中而作为诸如位错环的扩展缺陷D2a。通过这种热处理使微小缺陷核Dc1成长为微小缺陷D1。As shown in FIG. 6, an impurity element such as silicon or argon is introduced into p-type substrate PSB1 from above main surface S1 of p-type substrate PSB1 by employing a conventional ion implantation technique. Subsequently, the p-type substrate PSB1 is heat-treated again by a generally known method, so that introduced impurity elements such as silicon or argon are embedded in the substrate as extended defects D2a such as dislocation loops. The microdefect nuclei Dc1 are grown into microdefects D1 by such heat treatment.
采用离子注入技术引入的杂质元素的剂量优选是足以形成扩展缺陷的量,例如5E14cm-2以上。The dose of impurity elements introduced by the ion implantation technique is preferably an amount sufficient to form extended defects, for example, more than 5E14 cm −2 .
如图7中所示,由硅制成的第一p型外延层PE1通过典型的外延生长形成在p型衬底PSB1的主表面S1上(以便与主表面S1的上表面接触)。第一p型外延层PE1例如包含作为p型杂质的硼。硼的浓度例如优选设定为4E17cm-3以上但不大于1E20cm-3。第一p型外延层PE1的厚度优选设定为0.5μm以上但不大于3μm,更优选1μm以上但不大于2μm。As shown in FIG. 7 , a first p-type epitaxial layer PE1 made of silicon is formed on main surface S1 of p-type substrate PSB1 (so as to be in contact with the upper surface of main surface S1 ) by typical epitaxial growth. The first p-type epitaxial layer PE1 contains, for example, boron as a p-type impurity. The concentration of boron is preferably set to, for example, 4E17 cm -3 or more but not more than 1E20 cm -3 . The thickness of the first p-type epitaxial layer PE1 is preferably set to be 0.5 μm or more but not more than 3 μm, more preferably 1 μm or more but not more than 2 μm.
如图8中所示,形成由硅制成的第二p型外延层PE2以便覆盖第一p型外延层PE1的上表面。第二p型外延层PE2也例如包含硼的p型杂质。硼的浓度例如优选设定为5E14cm-3以上但不大于1E16cm-3。优选设定为等于p衬底PSB1中包含的硼的浓度。虽然第二p型外延层PE2的厚度决定来自由光电二极管PD1收集的红光的空穴电子的收集灵敏度并根据半导体成像器件的设计方案改变,但是在插入IR(红外)截止滤光器的可见光图像传感器的情况下,其基本上优选设定为2μm以上但不大于6μm,更优选3μm以上但不大于5μm。As shown in FIG. 8, the second p-type epitaxial layer PE2 made of silicon is formed so as to cover the upper surface of the first p-type epitaxial layer PE1. The second p-type epitaxial layer PE2 also contains, for example, a p-type impurity of boron. The concentration of boron is preferably set to, for example, 5E14 cm -3 or more but not more than 1E16 cm -3 . It is preferably set to be equal to the concentration of boron contained in the p-substrate PSB1. Although the thickness of the second p-type epitaxial layer PE2 determines the collection sensitivity of hole electrons from the red light collected by the photodiode PD1 and changes according to the design scheme of the semiconductor imaging device, in the visible light with an IR (infrared) cut filter inserted In the case of an image sensor, it is basically preferably set to 2 μm or more but not more than 6 μm, more preferably 3 μm or more but not more than 5 μm.
如上所述的微小缺陷D1以及注入引发的缺陷D2a的形成使p型衬底PSB1的缺陷密度高于第二p型外延层PE2的缺陷密度。The above-mentioned formation of the tiny defects D1 and the implant-induced defects D2a makes the defect density of the p-type substrate PSB1 higher than the defect density of the second p-type epitaxial layer PE2.
随后,在第二p型外延层PE2的上表面中形成浅凹槽。本文所用术语“浅凹槽”是指足够浅而没有到达第二p型外延层PE2下的第一p型外延层PE1的凹槽。优选形成例如具有150nm以上但不大于400nm深度的沟槽。凹槽形成在平面图中,分别围绕第一像素区RPx和第二像素区GPx(其中将要形成沟槽隔离TI的区域)的区域中。Subsequently, shallow grooves are formed in the upper surface of the second p-type epitaxial layer PE2. The term "shallow groove" as used herein refers to a groove shallow enough not to reach the first p-type epitaxial layer PE1 under the second p-type epitaxial layer PE2. It is preferable to form a trench having a depth of, for example, 150 nm or more but not more than 400 nm. Grooves are formed in regions respectively surrounding the first pixel region RPx and the second pixel region GPx (regions in which trench isolations TI are to be formed) in plan view.
随后,例如通过采用典型的CVD(化学气相沉积)以例如氧化硅膜的绝缘膜填充凹槽。利用CMP(化学机械抛光)移除第二p型外延层PE2上的绝缘膜。以此方式形成沟槽隔离TI。Subsequently, the groove is filled with an insulating film such as a silicon oxide film, for example, by employing typical CVD (Chemical Vapor Deposition). The insulating film on the second p-type epitaxial layer PE2 is removed by CMP (Chemical Mechanical Polishing). In this way, trench isolation TI is formed.
如图9中所示,通过采用典型光刻方法仅在由沟槽隔离TI围绕的第一像素区RPx中形成光刻胶PHR(感光体)的掩膜图案。可以形成这种掩膜图案以便包括第一像素区RPx和第二像素区GPx之间边界部的一部分。As shown in FIG. 9, a mask pattern of a photoresist PHR (photoreceptor) is formed only in the first pixel region RPx surrounded by the trench isolation TI by employing a typical photolithography method. Such a mask pattern may be formed so as to include a portion of a boundary portion between the first pixel region RPx and the second pixel region GPx.
随后,通过采用光刻胶PHR的掩膜图案,通过典型的离子注入形成第一注入区PJ1,以便覆盖在第二p型外延层PE2中并且在将要在第二像素区GPx中形成光电二极管PD2的区域下的第一p型外延层PE1的上表面。换言之,第一注入区PJ1形成在第二p型外延层PE2的最下部中(p型衬底PSB1一侧上),以便具有高于第二p型外延层PE2的p型杂质浓度。作为一个实例,当第二p型外延层PE2具有4μm厚度时,以2.3MeV的能量和2E13cm-2的剂量注入硼杂质。Subsequently, by using a mask pattern of photoresist PHR, a first implantation region PJ1 is formed by typical ion implantation so as to cover in the second p-type epitaxial layer PE2 and to form a photodiode PD2 in the second pixel region GPx The upper surface of the first p-type epitaxial layer PE1 under the region. In other words, the first implantation region PJ1 is formed in the lowermost portion of the second p-type epitaxial layer PE2 (on the p-type substrate PSB1 side) so as to have a higher p-type impurity concentration than the second p-type epitaxial layer PE2. As an example, when the second p-type epitaxial layer PE2 has a thickness of 4 μm, boron impurities are implanted at an energy of 2.3 MeV and a dose of 2E13 cm −2 .
如图10中所示,仅在各由沟槽隔离TI围绕的第一像素区RPx和第二像素区GPx中,利用典型光刻方法形成光刻胶PHR(感光体)的掩膜图案。在这种情况下,例如,随后通过典型的离子注入技术将硼引入沟槽隔离TI的正下方。因此,第二注入区PJ2形成在第二p型外延层PE2中的第一像素区RPx(其中将要形成光电二极管PD1的区域)和第二像素区GPx(其中将要形成光电二极管PD2的区域)之间的边界部处。As shown in FIG. 10, only in the first pixel region RPx and the second pixel region GPx each surrounded by the trench isolation TI, a mask pattern of a photoresist PHR (photoreceptor) is formed using a typical photolithography method. In this case, for example, boron is then introduced directly under the trench isolation TI by typical ion implantation techniques. Therefore, the second injection region PJ2 is formed between the first pixel region RPx (the region where the photodiode PD1 is to be formed) and the second pixel region GPx (the region where the photodiode PD2 is to be formed) in the second p-type epitaxial layer PE2 at the boundary between.
提供将被引入的硼以便穿透沟槽隔离TI并到达正下方的第二p型外延层PE2。对于引入硼来说,优选采用多级注入。更具体地,在引入作为杂质的硼的同时分级地改变能量,例如在200keV至2.0MeV之间。这使得能形成具有高于第二p型外延层PE2的p型杂质浓度的第二注入区PJ2,并且同时使第二注入区PJ2在第二注入区的最下部与第一注入区PJ1接触。而且,还可以形成第二注入区PJ2以在该区域的最上部与沟槽隔离TI接触。注入之后是图10的光刻胶PHR的移除。The boron to be introduced is provided to penetrate the trench isolation TI and reach the second p-type epitaxial layer PE2 directly below. For the introduction of boron, multi-stage implantation is preferably used. More specifically, the energy is changed stepwise, for example, between 200keV and 2.0MeV while introducing boron as an impurity. This makes it possible to form the second implantation region PJ2 having a higher p-type impurity concentration than the second p-type epitaxial layer PE2 while bringing the second implantation region PJ2 into contact with the first implantation region PJ1 at the lowermost portion of the second implantation region. Also, a second implantation region PJ2 may also be formed to contact the trench isolation TI at the uppermost portion of the region. Implantation is followed by removal of the photoresist PHR of FIG. 10 .
如图4中所示,通过典型的光刻方法并且通过将p型杂质元素注入沟槽隔离TI的底部以及沟槽隔离TI的侧部以在将要形成的光电二极管PD1和PD2的相应侧上形成保护环GR。As shown in FIG. 4, by a typical photolithography method and by implanting p-type impurity elements into the bottom of the trench isolation TI and the sides of the trench isolation TI to form on the respective sides of the photodiodes PD1 and PD2 to be formed Guard ring GR.
随后,分别在所需位置形成栅极绝缘膜GI和转移栅Tx。更具体地,通过热氧化处理在第二p型外延层PE2的上表面上形成栅极绝缘膜GI。在栅极绝缘膜GI上沉积将作为转移栅Tx的多晶硅膜等而作为栅电极。随后,将栅极绝缘膜GI和多晶硅等图案化成如图4中所示的栅极绝缘膜GI和转移栅Tx。Subsequently, a gate insulating film GI and a transfer gate Tx are formed at desired positions, respectively. More specifically, a gate insulating film GI is formed on the upper surface of the second p-type epitaxial layer PE2 by thermal oxidation treatment. A polysilicon film or the like to be a transfer gate Tx is deposited on the gate insulating film GI as a gate electrode. Subsequently, the gate insulating film GI and polysilicon and the like are patterned into the gate insulating film GI and the transfer gate Tx as shown in FIG. 4 .
随后,在图4的转移栅Tx的左侧上的区域中,利用典型的光刻方法和离子注入技术形成n型杂质区。因此,光电二极管PD1形成在第一像素区RPx中且光电二极管PD2形成在第二像素区GPx中,因此它们在沿p型衬底PSB1的主表面S1的方向上布置在第二p型外延层PE2中。因此第一和第二像素区RPx和GPx在图4的转移栅Tx的右侧上的区域中具有电容区FD。光电二极管PD1和PD2形成在相邻于保护环GR的位置处。Subsequently, in a region on the left side of the transfer gate Tx of FIG. 4, an n-type impurity region is formed using a typical photolithography method and ion implantation technique. Therefore, the photodiode PD1 is formed in the first pixel region RPx and the photodiode PD2 is formed in the second pixel region GPx, so they are arranged in the direction along the main surface S1 of the p-type substrate PSB1 on the second p-type epitaxial layer In PE2. Therefore, the first and second pixel regions RPx and GPx have a capacitance region FD in a region on the right side of the transfer gate Tx of FIG. 4 . Photodiodes PD1 and PD2 are formed at positions adjacent to the guard ring GR.
虽未说明滤光器,但是第一像素区RPx具备红色滤光器并且第二像素区GPx具备绿色或蓝色滤光器。光电二极管PD2接收具有短于光电二极管PD1的平均波长的光。Although filters are not illustrated, the first pixel region RPx is provided with a red filter and the second pixel region GPx is provided with a green or blue filter. The photodiode PD2 receives light having an average wavelength shorter than that of the photodiode PD1.
光电二极管PD1和PD2在其正上方具有通过采用典型的光刻方法和离子注入技术形成的n型杂质区,并且因此具有表面p型区SPR。The photodiodes PD1 and PD2 have n-type impurity regions directly thereon formed by employing typical photolithography methods and ion implantation techniques, and thus have surface p-type regions SPR.
最后,利用一般公知方法执行热处理以形成如图4中所示的结构。随后,将参考图11的比较实例和图12至15的曲线图说明本实施例的效果和优点。Finally, heat treatment is performed using a generally known method to form a structure as shown in FIG. 4 . Subsequently, effects and advantages of the present embodiment will be described with reference to the comparative example of FIG. 11 and the graphs of FIGS. 12 to 15 .
如图11中所示,构成作为比较实例的半导体器件的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移栅TMI的构造具有以下不同。具体来说,在图11中,采用n型衬底NSB替代p型衬底PSB1(但是允许采用p型衬底PSB1)。替代图4的第一p型外延层PE1,采用离子注入技术形成第一注入区PJ1。替代图4的第二p型外延层PE2,第一注入区PJ1在其上具有通过离子注入技术形成的第三注入区PJ3,并且第三注入区PJ3在其中具有光电二极管PD1和PD2等。在第一像素区RPx和第二像素区GPx之间的边界处采用离子注入技术形成第二注入区PJ2,以便到达第一注入区PJ1。As shown in FIG. 11 , the configurations of a photodiode PD of a semiconductor imaging device constituting a semiconductor device as a comparative example and a transfer gate TMI including the photodiode PD have the following differences. Specifically, in FIG. 11, the n-type substrate NSB is used instead of the p-type substrate PSB1 (but the p-type substrate PSB1 is allowed to be used). Instead of the first p-type epitaxial layer PE1 of FIG. 4 , the first implantation region PJ1 is formed by ion implantation technology. Instead of the second p-type epitaxial layer PE2 of FIG. 4 , the first implantation region PJ1 has thereon a third implantation region PJ3 formed by an ion implantation technique, and the third implantation region PJ3 has photodiodes PD1 and PD2 etc. therein. The second implantation region PJ2 is formed using an ion implantation technique at the boundary between the first pixel region RPx and the second pixel region GPx so as to reach the first implantation region PJ1.
在本实施例中,采用外延生长形成p型外延层PE1和PE2。另一方面,在比较实例中,采用离子注入技术分别形成对应于它们的注入区PJ1和PJ3,但是它们由类似于本实施例的硅制成。In this embodiment, the p-type epitaxial layers PE1 and PE2 are formed by epitaxial growth. On the other hand, in the comparative example, the implanted regions PJ1 and PJ3 corresponding to them were respectively formed using the ion implantation technique, but they were made of silicon similar to the present embodiment.
如图12所示,沿横坐标绘制入射在光电二极管上的光波长(nm),同时在纵坐标上作为光吸收比(纵坐标上采用任意单位)绘制通过在半导体成像器件中已经被光电二极管接收的光的光电转换而产生的电子的吸收比。应当注意光电二极管形成在硅中。As shown in Figure 12, the light wavelength (nm) incident on the photodiode is plotted along the abscissa, while the light absorption ratio (arbitrary unit is adopted on the ordinate) is plotted by the photodiode in the semiconductor imaging device on the ordinate. Absorption ratio of electrons generated by photoelectric conversion of received light. It should be noted that the photodiodes are formed in silicon.
由图12显而易见的是与收集区从光电二极管的表面延伸至浅区(2μm)相比,当收集区从形成表面延伸至深位置(4μm)时,通过具有特别长波长的(R(红))光的光电转换而产生的电子以非常高的比率被光电二极管收集。另一方面,当收集由具有短波长的(G(绿))光的光电转换而产生的电子时,在从表面仅延伸至较浅位置的收集区和从表面延伸至较深位置的收集区之间没有大的差异。在上述两种情况下,与由具有长波长的光产生的电子相比,电子都能以相对高的比率被光电二极管收集。It is apparent from FIG. 12 that when the collection region extends from the formation surface to a deep position (4 μm) compared to the collection region extending from the surface of the photodiode to a shallow region (2 μm), passing through the (R (red) ) electrons generated by photoelectric conversion of light are collected by photodiodes at a very high rate. On the other hand, when electrons generated by photoelectric conversion of (G (green)) light having a short wavelength are collected, in the collection region extending from the surface only to a shallower position and in the collection region extending from the surface to a deeper position There is no big difference between. In both cases described above, electrons can be collected by the photodiode at a relatively high rate compared with electrons generated by light having a long wavelength.
简言之,希望接收具有特别长波长的光,即红光的光电二极管容易在从半导体成像器件的表面起的深位置处收集由光电转换而产生的电子。换言之,希望用于红光的光电二极管在从半导体成像器件的表面起的深位置处具有对由光电转换而产生的电子的高灵敏度。In short, it is desired that a photodiode that receives light having a particularly long wavelength, ie, red light, easily collects electrons generated by photoelectric conversion at a deep position from the surface of the semiconductor imaging device. In other words, a photodiode for red light is expected to have high sensitivity to electrons generated by photoelectric conversion at a deep position from the surface of the semiconductor imaging device.
与短波长光相比,长波长光可能穿透进入半导体成像器件中的更深的位置。允许通过光电转换而产生在较深位置处收集电子的构造可提高光电二极管对于长波长光的灵敏度。Long-wavelength light may penetrate deeper into a semiconductor imaging device than short-wavelength light. A configuration that allows collection of electrons at a deeper position by photoelectric conversion can improve the sensitivity of the photodiode to long-wavelength light.
当采用离子注入技术形成其中如图11中所示形成接收长波长光的光电二极管PD1的p型区PJ3时,p型区PJ3不能具有大深度(如图11的第一注入区PJ1那样,有时通过离子注入技术在较深区域中形成薄膜,但是这取决于由此形成的区域的厚度或宽度),因为离子注入技术不适于形成从表面延伸至相对深区域的杂质区。When the ion implantation technique is used to form the p-type region PJ3 in which the photodiode PD1 receiving long-wavelength light is formed as shown in FIG. A thin film is formed in a deeper region by ion implantation technology, but it depends on the thickness or width of the region thus formed), because ion implantation technology is not suitable for forming an impurity region extending from the surface to a relatively deep region.
因此,如图4所示,通过外延生长替代p型区PJ3而形成p型区PE2。因为通过外延生长形成的第二p型外延层PE2的厚度相对于通过离子注入技术形成的p型区PJ3而自由控制,因此可以形成从表面延伸至相对较深的区域的p型杂质区。这意味着图4的第二p型外延层PE2能比图11的第三注入区PJ3延伸至更深的位置。因此可以通过光电二极管PD1以高灵敏度收集已经发生在p型杂质区PE2的特别深的区域中的光电转换而产生的电子。因此,光电二极管PD1可以具有相对于电子的增强的灵敏度。Therefore, as shown in FIG. 4, p-type region PE2 is formed by epitaxial growth instead of p-type region PJ3. Since the thickness of the second p-type epitaxial layer PE2 formed by epitaxial growth is freely controlled relative to the p-type region PJ3 formed by ion implantation technology, a p-type impurity region extending from the surface to a relatively deep region can be formed. This means that the second p-type epitaxial layer PE2 in FIG. 4 can extend to a deeper position than the third implantation region PJ3 in FIG. 11 . Electrons generated by photoelectric conversion that have occurred in a particularly deep region of the p-type impurity region PE2 can therefore be collected with high sensitivity by the photodiode PD1. Therefore, the photodiode PD1 may have enhanced sensitivity with respect to electrons.
此外,因为采用外延生长形成p型外延层PE2,可以使p型外延层PE2中包含的残留缺陷密度小于相应地通过离子注入技术形成的区域中包含的残留缺陷密度。这使得光电二极管PD1以更高比率收集产生在p型外延层PE2中产生的电子。In addition, since the p-type epitaxial layer PE2 is formed by epitaxial growth, the density of residual defects contained in the p-type epitaxial layer PE2 can be made smaller than that contained in regions correspondingly formed by ion implantation techniques. This allows the photodiode PD1 to collect electrons generated in the p-type epitaxial layer PE2 at a higher rate.
在图13中,该柱状图示出图11中所示的比较实例以及图4中所示的本实施例的半导体成像器件中通过红光(具有635nm的波长)的光电转换产生的电子以及通过绿光(具有530nm的波长)的光电转换产生的电子中每一个的内部量子效率(纵坐标为任意单位)。本文所用的术语“内部量子效率”是指由光电二极管收集的通过转换获得的电子的收集比率。In FIG. 13, the histogram shows electrons generated by photoelectric conversion of red light (having a wavelength of 635 nm) and electrons generated by photoelectric conversion in the comparative example shown in FIG. 11 and the semiconductor imaging device of the present embodiment shown in FIG. The internal quantum efficiency (arbitrary units on the ordinate) of each of the electrons generated by the photoelectric conversion of green light (with a wavelength of 530 nm). The term "internal quantum efficiency" as used herein refers to the collection ratio of electrons obtained by conversion collected by a photodiode.
由图13特别显而易见的是,如本实施例中那样,通过形成具有比比较实例的第三注入区PJ3的深度更深的深度的第二p型外延层PE2,能大幅提高由红光的光电转换而产生的电子的收集效率。也少量提高了由绿光的光电转换而产生的电子的收集效率。It is particularly apparent from FIG. 13 that, as in this embodiment, by forming the second p-type epitaxial layer PE2 having a depth deeper than that of the third injection region PJ3 of the comparative example, photoelectric conversion by red light can be greatly improved. The resulting electron collection efficiency. The collection efficiency of electrons generated by photoelectric conversion of green light is also slightly improved.
从图14中也能显而易见的是,如图14的曲线图中所示,沿横坐标绘制第二p型外延层PE2的厚度(μm)并且沿纵坐标绘制例如通过红光的光电转换而产生的电子的内部量子效率(纵坐标为任意单位)。图14暗示电子的收集效率随第二p型外延层PE2的厚度(μm)的增大而增大。It can also be apparent from FIG. 14 that, as shown in the graph of FIG. 14 , the thickness (μm) of the second p-type epitaxial layer PE2 is plotted along the abscissa and the thickness (μm) of the second p-type epitaxial layer PE2 is plotted along the ordinate such as that produced by photoelectric conversion of red light. The internal quantum efficiency of the electrons (the ordinate is in arbitrary units). FIG. 14 suggests that the collection efficiency of electrons increases as the thickness (μm) of the second p-type epitaxial layer PE2 increases.
长波长的红光可能更深地穿透进入薄膜和衬底中,因此会在第二p型外延层PE2下方的半导体衬底SUB中发生光电转换。当这种半导体衬底SUB是n型衬底NSB时,例如与图11的比较实例相同,在n型衬底NSB中可以高比率收集由n型半导体衬底NSB中的长波长光的光电转换而产生的电子,因为n型衬底与p型衬底相比具有容易收集电子的性质。这致使通过光电二极管PD1收集的电子的比率降低,从而导致光电二极管PD1对于电子的灵敏度的劣化。The long-wavelength red light may penetrate deeper into the film and the substrate, so photoelectric conversion may occur in the semiconductor substrate SUB under the second p-type epitaxial layer PE2. When this semiconductor substrate SUB is an n-type substrate NSB, for example, the same as the comparative example of FIG. The electrons generated because the n-type substrate has the property of easily collecting electrons compared with the p-type substrate. This causes a decrease in the rate of electrons collected by the photodiode PD1, resulting in deterioration of the sensitivity of the photodiode PD1 to electrons.
例如,如图4的本实施例中那样,利用p型衬底PSB1,因此可以抑制由这种衬底收集电子并增强对于由已经发生在衬底中的光电转换产生的电子的灵敏度。For example, as in the present embodiment of FIG. 4 , a p-type substrate PSB1 is used, so it is possible to suppress collection of electrons by such a substrate and enhance sensitivity to electrons generated by photoelectric conversion that has occurred in the substrate.
p型衬底PSB1形成在第一像素区RPx和第二像素区GPx的正下方,因此例如在第一像素区RPx的正下方的p型衬底PSB1中,由光电二极管PD1已经接收的光产生的电子容易进入与其相邻的第二像素区GPx。随后,可以通过光电二极管PD2收集由入射在光电二极管PD1上的光产生的电子。这种现象被称为“电子串扰”,并且其会导致光电二极管PD1和PD2的电子检测灵敏度的劣化以及混色。这意味着仅以p型衬底PSB1替代n型衬底NSB会增大p型衬底PSB1中的电子串扰,这会导致光电二极管PD1和PD2的电子检测灵敏度的劣化以及混色。The p-type substrate PSB1 is formed directly below the first pixel region RPx and the second pixel region GPx, so for example, in the p-type substrate PSB1 directly below the first pixel region RPx, light that has been received by the photodiode PD1 generates The electrons easily enter the second pixel region GPx adjacent thereto. Subsequently, electrons generated by light incident on the photodiode PD1 may be collected by the photodiode PD2. This phenomenon is called "electron crosstalk", and it causes deterioration of the electron detection sensitivity of the photodiodes PD1 and PD2 and color mixing. This means that merely substituting the p-type substrate PSB1 for the n-type substrate NSB increases electron crosstalk in the p-type substrate PSB1 , which leads to degradation of electron detection sensitivity and color mixing of photodiodes PD1 and PD2 .
而且,当输入超过饱和信号水平的水平的光信号时,存在模糊现象的可能性,即导致光电子没有被应该收集它们的光电二极管收集而是被与其相邻的另一光电二极管收集。Also, when an optical signal at a level exceeding the saturation signal level is input, there is a possibility of a blur phenomenon that causes photoelectrons not to be collected by a photodiode that should collect them but by another photodiode adjacent thereto.
增厚第二p型外延层PE2以提高光电二极管PD1的内部量子效率会增大电子串扰的可能性。Thickening the second p-type epitaxial layer PE2 to increase the internal quantum efficiency of the photodiode PD1 increases the possibility of electron crosstalk.
在图15中,本曲线图的横坐标,类似于图14的曲线图的横坐标,示出膜厚。在以图15中的实线示出的曲线图的各个实线中,沿纵坐标绘制例如由红光产生的电子的内部量子效率(纵坐标为任意单位)。在以图15中的虚线示出的曲线图的各个线中,沿纵坐标绘制电子串扰,即在不期望的光电二极管中对例如由红光的光电转换产生的电子的收集比率。In FIG. 15 , the abscissa of this graph, similar to that of the graph of FIG. 14 , shows the film thickness. In each solid line of the graph shown with a solid line in FIG. 15 , the internal quantum efficiency of, for example, electrons generated by red light is plotted along the ordinate (the ordinate is in arbitrary units). In the respective lines of the graph shown with dotted lines in FIG. 15 , the electron crosstalk, ie the collection ratio of electrons resulting, for example, from photoelectric conversion of red light in an undesired photodiode is plotted along the ordinate.
图15中以实线和正方形示出的曲线图与图14的曲线图相同,而图15中以虚线和正方形示出的曲线图示出在类似于图14的曲线图的情况下的电子串扰的发生比率。它们是在“没有位错环”的情况下绘制的,意味着没有故意形成注入引起的缺陷D2a。第二p型外延层PE2的厚度的增大以提高内部量子效率往往会增大电子串扰的发生比率,假设其由更深区域中的p型衬底PSB1中的光电转换的发生比率的增大引起。The graph shown with solid lines and squares in FIG. 15 is the same as the graph of FIG. 14 , while the graph shown with dashed lines and squares in FIG. 15 shows electronic crosstalk in a situation similar to the graph of FIG. 14 incidence rate. They were drawn "without dislocation loops", meaning that no injection-induced defect D2a was intentionally formed. An increase in the thickness of the second p-type epitaxial layer PE2 to increase the internal quantum efficiency tends to increase the occurrence ratio of electron crosstalk, which is assumed to be caused by an increase in the occurrence ratio of photoelectric conversion in the p-type substrate PSB1 in the deeper region .
在本实施例中,通过采用图5和6中所示的方法,将半导体衬底SUB转化成p型衬底PSB1,即,含p型杂质的衬底,并且同时,使p型衬底PSB1的缺陷密度高于第二p型外延层PE2的缺陷密度。更具体地,许多诸如位错环的注入引发的缺陷D2a以及来源于氧的BMD的微小缺陷D1预先形成在p型衬底PSB1中。随后,由于这些缺陷而使p型衬底PSB1中产生的电子发生复合并消失在p型衬底PSB1中,因此大幅降低电子的载流子寿命。这使得能减少造成电子串扰的p型衬底PSB1中产生的电子的可能性。因此,由于故意形成的缺陷D1和D2,因此可以使p型衬底PSB1中产生的电子通过复合而有效地消失。In this embodiment, by using the method shown in FIGS. 5 and 6, the semiconductor substrate SUB is converted into a p-type substrate PSB1, that is, a substrate containing p-type impurities, and at the same time, the p-type substrate PSB1 is made The defect density of is higher than the defect density of the second p-type epitaxial layer PE2. More specifically, many microscopic defects D1 such as implantation-induced defects D2a of dislocation loops and oxygen-derived BMDs are preliminarily formed in the p-type substrate PSB1. Subsequently, the electrons generated in the p-type substrate PSB1 are recombined due to these defects and disappear in the p-type substrate PSB1, thereby greatly reducing the carrier lifetime of the electrons. This makes it possible to reduce the possibility of electrons generated in the p-type substrate PSB1 causing electron crosstalk. Therefore, electrons generated in the p-type substrate PSB1 can be effectively eliminated by recombination due to the intentionally formed defects D1 and D2.
再次参考图15,当诸如位错环的注入引发的缺陷D2a故意形成在p型衬底PSB1中(曲线图中的“位错环”),与没有形成缺陷时相比降低了电子串扰的发生比率。当控制衬底中的氧浓度时,进一步降低电子串扰的发生比率,并且由此也控制将在下文说明的通过微小缺陷D1形成在衬底中的复合缺陷密度D2b(曲线图中的“衬底寿命控制”)。Referring again to FIG. 15 , when implantation-induced defects D2a such as dislocation loops are intentionally formed in the p-type substrate PSB1 (“dislocation loops” in the graph), the occurrence of electronic crosstalk is reduced compared to when no defects are formed. ratio. When the oxygen concentration in the substrate is controlled, the occurrence ratio of electron crosstalk is further reduced, and thus also the composite defect density D2b formed in the substrate by the minute defect D1 to be described later ("substrate" in the graph) is controlled. Life Control").
简言之,在本实施例中,通过允许光电二极管PD1以高比率有效收集由第二p型外延层PE2中的光电转换产生的电子,并且相反,允许p型衬底PSB1中由光电转换产生的电子快速消失,可以实现折衷关系的两个目的,即高内部量子效率和低电子串扰。In short, in this embodiment, electrons generated by photoelectric conversion in the second p-type epitaxial layer PE2 are efficiently collected by allowing the photodiode PD1 to efficiently collect electrons generated by photoelectric conversion in the second p-type epitaxial layer PE2, and conversely, allowing electrons generated by photoelectric conversion in the p-type substrate PSB1 The rapid disappearance of the electrons can achieve the two purposes of the trade-off relationship, that is, high internal quantum efficiency and low electron crosstalk.
在本实施例中,第一p型外延层PE1夹在p型衬底PSB1和第二p型外延层PE2之间,并且第一p型外延层PE1用作p型衬底PSB1和第二p型外延层PE2之间的边界部。此外,第一p型外延层PE1具有高于第二p型外延层PE2的p型杂质浓度。因此第一p型外延层PE1用作用于抑制p型衬底PSB1中产生的电子进入第二p型外延层PE2的势垒。In this embodiment, the first p-type epitaxial layer PE1 is sandwiched between the p-type substrate PSB1 and the second p-type epitaxial layer PE2, and the first p-type epitaxial layer PE1 serves as the p-type substrate PSB1 and the second p-type epitaxial layer PE1. Type epitaxial layer PE2 between the boundary portion. In addition, the first p-type epitaxial layer PE1 has a higher p-type impurity concentration than the second p-type epitaxial layer PE2. The first p-type epitaxial layer PE1 thus functions as a potential barrier for suppressing electrons generated in the p-type substrate PSB1 from entering the second p-type epitaxial layer PE2.
这还适用于具有设定为高于第二p型外延层PE2的p型杂质浓度的第一注入区PJ1和第二注入区PJ2。例如,第一注入区PJ1在第二像素区GPx中用作用于抑制电子从p型衬底PSB1进入第二p型外延层PE2的势垒。第二注入区PJ2用作用于抑制已经通过光电转换而获得的电子在第二p型外延层PE2中在第一像素区RPx和第二像素区GPx之间移动的势垒。This also applies to the first implantation region PJ1 and the second implantation region PJ2 having the p-type impurity concentration set higher than that of the second p-type epitaxial layer PE2. For example, the first injection region PJ1 functions as a barrier for suppressing entry of electrons from the p-type substrate PSB1 into the second p-type epitaxial layer PE2 in the second pixel region GPx. The second injection region PJ2 functions as a potential barrier for suppressing movement of electrons that have been obtained through photoelectric conversion between the first pixel region RPx and the second pixel region GPx in the second p-type epitaxial layer PE2.
第二注入区PJ2在第一注入区PJ1的上表面处与其接触,因此在第一注入区PJ1和第二注入区PJ2彼此邻接的区域中,这些区域彼此连接并且这些区域之间没有形成间隔(没有形成注入区)。第一像素区RPx和第二像素区GPx中每一个的第二p型外延层PE2在外延层下方都由注入区PJ1和PJ2完全围绕,因此注入区PJ1和PJ2抑制了电子串扰,使得能够进一步提高用于收集通过光电二极管PD1的光电转换获得的电子的光电二极管PD1的灵敏度。The second implantation region PJ2 is in contact with the first implantation region PJ1 at the upper surface thereof, so that in regions where the first implantation region PJ1 and the second implantation region PJ2 adjoin each other, these regions are connected to each other and no space is formed between these regions ( no injection region is formed). The second p-type epitaxial layer PE2 of each of the first pixel region RPx and the second pixel region GPx is completely surrounded by the injection regions PJ1 and PJ2 below the epitaxial layer, so the injection regions PJ1 and PJ2 suppress electron crosstalk, enabling further The sensitivity of the photodiode PD1 for collecting electrons obtained by photoelectric conversion of the photodiode PD1 is increased.
假设第二注入区PJ2在其上表面处与沟槽隔离TI接触,则第一像素区RPx和第二像素区GPx的第二p型外延层PE2在外延层的上部和下部处完全由注入区PJ1和PJ2围绕。这进一步增强了注入区PJ1和PJ2的电子串扰抑制效果。Assuming that the second implantation region PJ2 is in contact with the trench isolation TI at its upper surface, the second p-type epitaxial layer PE2 of the first pixel region RPx and the second pixel region GPx is completely formed by the implantation region at the upper and lower parts of the epitaxial layer. PJ1 and PJ2 surround. This further enhances the electronic crosstalk suppression effect of the injection regions PJ1 and PJ2.
虽然第一注入区PJ1形成为覆盖第二像素区GPx中的第一p型外延层PE1的上表面,第一注入区PJ1没有形成在第一像素区RPx中。这意味着在具有光电转换元件,例如接收具有相对长波长的光电二极管PD1的像素区中,没有形成覆盖第一p型外延层PE1的上表面的第一注入区PJ1。因此第二像素区GPx中的第二p型外延层PE2的表观厚度小于第一像素区RPx中的情况。能接收短波长光的第二像素区GPx的光电二极管PD2可以高比率收集浅区域中通过光电转换获得的电子,因此没有发生功能问题。Although the first injection region PJ1 is formed to cover the upper surface of the first p-type epitaxial layer PE1 in the second pixel region GPx, the first injection region PJ1 is not formed in the first pixel region RPx. This means that in a pixel region having a photoelectric conversion element such as a photodiode PD1 receiving a relatively long wavelength, the first injection region PJ1 covering the upper surface of the first p-type epitaxial layer PE1 is not formed. Therefore, the apparent thickness of the second p-type epitaxial layer PE2 in the second pixel region GPx is smaller than that in the first pixel region RPx. The photodiode PD2 of the second pixel region GPx capable of receiving short-wavelength light can collect electrons obtained by photoelectric conversion in a shallow region at a high rate, and thus no functional problem occurs.
在本实施例中,第一p型外延层PE1和第二p型外延层PE2由相同材料制成,即硅,因此可以减小它们之间界面处产生泄漏电流的可能性。In this embodiment, the first p-type epitaxial layer PE1 and the second p-type epitaxial layer PE2 are made of the same material, namely silicon, so the possibility of leakage current at the interface between them can be reduced.
(第二实施例)(second embodiment)
首先,参考图16,将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移晶体管TMI的构造。First, with reference to FIG. 16 , configurations of a photodiode PD constituting a semiconductor imaging device as a semiconductor device of the present embodiment and a transfer transistor TMI including the photodiode PD will be described in detail.
图16是示出与图4中所示的第一实施例相同的区域的模式的示意截面图。如图16所示,本实施例具有基本上类似于图4中所示的第一实施例的构造,但以下要点与第一实施例不同。Fig. 16 is a schematic cross-sectional view showing a pattern of the same region as that of the first embodiment shown in Fig. 4 . As shown in FIG. 16, this embodiment has a configuration basically similar to that of the first embodiment shown in FIG. 4, but differs from the first embodiment in the following points.
具体来说,在本实施例中,第一p型外延层PE1由多个彼此不同的p型外延层构成。其从p型衬底PSB1一侧具有依序由重掺杂p型外延层PE1a,轻掺杂p型外延层PE1b以及重掺杂p型外延层PE1c的堆叠膜。重掺杂p型外延层PE1a以及重掺杂p型外延层PE1c中的p型杂质浓度高于第二p型外延层PE2中的p型杂质浓度。例如其基本上等于第一实施例的第一p型外延层PE1中的p型杂质浓度。轻掺杂p型外延层PE1b中的p型杂质浓度基本上等于第二p型外延层PE2中的p型杂质浓度。Specifically, in this embodiment, the first p-type epitaxial layer PE1 is composed of a plurality of different p-type epitaxial layers. From the p-type substrate PSB1 side, it has a stacked film sequentially composed of heavily doped p-type epitaxial layer PE1a, lightly doped p-type epitaxial layer PE1b and heavily doped p-type epitaxial layer PE1c. The p-type impurity concentration in the heavily doped p-type epitaxial layer PE1a and the heavily doped p-type epitaxial layer PE1c is higher than the p-type impurity concentration in the second p-type epitaxial layer PE2. For example, it is substantially equal to the p-type impurity concentration in the first p-type epitaxial layer PE1 of the first embodiment. The p-type impurity concentration in the lightly doped p-type epitaxial layer PE1b is substantially equal to the p-type impurity concentration in the second p-type epitaxial layer PE2.
布置在最靠近p型衬底PSB1一侧上的重掺杂p型外延层PE1a(衬底邻接层)具有复合缺陷D2b(第一扩展缺陷)。复合缺陷D2b由于在重掺杂p型外延层PE1a中例如重掺杂p型外延层PE1a中的硼的p型杂质与从相邻于重掺杂p型外延层PE1a的p型衬底PSB1扩散进入p型外延层PE1a的氧沉淀核(例如构成微小缺陷D1的那些)之间的反应而形成。The heavily doped p-type epitaxial layer PE1a (substrate-adjacent layer) disposed on the side closest to the p-type substrate PSB1 has composite defects D2b (first extended defects). The composite defect D2b is due to the p-type impurity in the heavily doped p-type epitaxial layer PE1a, such as boron in the heavily doped p-type epitaxial layer PE1a, diffused from the p-type substrate PSB1 adjacent to the heavily doped p-type epitaxial layer PE1a Formed by a reaction between oxygen precipitation nuclei (for example, those constituting minute defects D1) entering the p-type epitaxial layer PE1a.
简言之,从包含用于形成复合缺陷D2b的高浓度的p型杂质(硼)以及有助于尽可能地与p型衬底PSB1中的氧核结合的观点来看,作为最下层的重掺杂p型外延层PE1a形成在相邻于p型衬底PSB1的位置处。In short, from the viewpoint of containing a high concentration of p-type impurities (boron) for forming composite defects D2b and contributing to bonding with oxygen nuclei in the p-type substrate PSB1 as much as possible, the heavy The doped p-type epitaxial layer PE1a is formed at a position adjacent to the p-type substrate PSB1.
在构成第一p型外延层PE1的层之中,布置在最靠近p型衬底PSB1一侧上的重掺杂p型外延层PE1a中的氧浓度高于除重掺杂p型外延层PE1a之外构成第一p型外延层PE1的层中的氧浓度。Among the layers constituting the first p-type epitaxial layer PE1, the oxygen concentration in the heavily doped p-type epitaxial layer PE1a disposed on the side closest to the p-type substrate PSB1 is higher than that of the heavily doped p-type epitaxial layer PE1a. Oxygen concentration in layers constituting the first p-type epitaxial layer PE1.
作为最上层的重掺杂p型外延层PE1c具有类似于第一实施例中的第一p型外延层PE1的作用。具体来说,其分隔p型衬底PSB1和第二p型外延层PE2并布置为抑制它们之间的电子的自由迁移。夹在p型外延层PE1a和p型外延层PE1c之间的轻掺杂p型外延层PE1b具有它们之间的缓冲层的作用。The heavily doped p-type epitaxial layer PE1c as the uppermost layer has a role similar to that of the first p-type epitaxial layer PE1 in the first embodiment. Specifically, it separates the p-type substrate PSB1 and the second p-type epitaxial layer PE2 and is arranged to suppress free movement of electrons between them. The lightly doped p-type epitaxial layer PE1b sandwiched between the p-type epitaxial layer PE1a and the p-type epitaxial layer PE1c functions as a buffer layer therebetween.
除上述外延层之外的本实施例的构造基本类似于图4中所示的第一实施例,因此相同部件由相同参考符号表示并且省略重复说明。The configuration of this embodiment other than the above-described epitaxial layer is basically similar to that of the first embodiment shown in FIG. 4 , and thus the same components are denoted by the same reference symbols and repeated explanations are omitted.
参考图17至21,将说明制造构成作为本实施例的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移晶体管TMI的方法。图17至21示出与图16相同的区域的处理。Referring to FIGS. 17 to 21 , a method of manufacturing the photodiode PD constituting the semiconductor imaging device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described. 17 to 21 show processing of the same area as in FIG. 16 .
如图17所示,通过典型的外延生长在如第一实施例中提供的p型衬底PSB1的主表面上形成包括多个层的第一p型外延层PE1。本文所用术语“多个层”例如是指通过从靠近p型衬底PSB1一侧依次堆叠重掺杂p型外延层PE1a,轻掺杂p型外延层PE1b以及重掺杂p型外延层PE1c而获得的三层。重掺杂p型外延层PE1a和PE1c各包含作为p型杂质的硼,并且浓度等于第一实施例的第一p型外延层PE1中的硼的浓度。更具体地,硼的浓度例如优选设定为4E17cm-3以上但不大于1E20cm-3。轻掺杂p型外延层PE1b包含作为p型杂质的硼,并且浓度等于第一实施例的第二p型外延层PE2中的硼的浓度。更具体地,硼的浓度例如优选设定为5E14cm-3以上但不大于1E16cm-3。As shown in FIG. 17, a first p-type epitaxial layer PE1 including a plurality of layers is formed on the main surface of the p-type substrate PSB1 as provided in the first embodiment by typical epitaxial growth. The term "plurality of layers" used herein refers to, for example, stacking a heavily doped p-type epitaxial layer PE1a, a lightly doped p-type epitaxial layer PE1b, and a heavily doped p-type epitaxial layer PE1c sequentially from the side close to the p-type substrate PSB1. Get three layers. The heavily doped p-type epitaxial layers PE1a and PE1c each contain boron as a p-type impurity, and the concentration is equal to the concentration of boron in the first p-type epitaxial layer PE1 of the first embodiment. More specifically, the concentration of boron is preferably set to, for example, 4E17 cm -3 or more but not more than 1E20 cm -3 . The lightly doped p-type epitaxial layer PE1b contains boron as a p-type impurity, and has a concentration equal to that of boron in the second p-type epitaxial layer PE2 of the first embodiment. More specifically, the concentration of boron is preferably set to, for example, 5E14 cm -3 or more but not more than 1E16 cm -3 .
在构成第一p型外延层PE1的层之中,布置在最靠近p型衬底PSB1一侧上的重掺杂p型外延层PE1a中的氧浓度被设定为高于除重掺杂p型外延层PE1a之外的构成第一p型外延层PE1的层中的氧浓度。在这个过程中,可以通过热处理使微小缺陷核Dc1生长为微小缺陷D1。Among the layers constituting the first p-type epitaxial layer PE1, the oxygen concentration in the heavily doped p-type epitaxial layer PE1a disposed on the side closest to the p-type substrate PSB1 is set to be higher than that of the heavily doped p-type epitaxial layer PE1a. The oxygen concentration in the layers constituting the first p-type epitaxial layer PE1a other than the p-type epitaxial layer PE1a. In this process, the minute defect core Dc1 can be grown into a minute defect D1 by heat treatment.
参考图18,对图17中形成的结构热处理。通过这种热处理,p型衬底PSB1中包含的氧(包括微小缺陷D1)扩散进入重掺杂p型外延层PE1a。通过这种扩散,重掺杂p型外延层PE1a中包含的氧(包括微小缺陷D1)与硼,即,引入重掺杂p型外延层PE1a中的p型杂质反应,从而在重掺杂p型外延层PE1a中形成复合缺陷D2b。Referring to FIG. 18, the structure formed in FIG. 17 is heat treated. Through this heat treatment, oxygen contained in the p-type substrate PSB1 (including minute defects D1) diffuses into the heavily doped p-type epitaxial layer PE1a. Through this diffusion, oxygen contained in the heavily doped p-type epitaxial layer PE1a (including minute defects D1) reacts with boron, that is, the p-type impurity introduced into the heavily doped p-type epitaxial layer PE1a, thereby The composite defect D2b is formed in the type epitaxial layer PE1a.
如图19至21所示,通过执行类似于图8至10中所示的第一实施例的处理,并且随后执行类似于图10中所示的第一实施例的后续步骤,形成图16中所示的结构。As shown in FIGS. 19 to 21, by performing processing similar to the first embodiment shown in FIGS. 8 to 10, and then performing subsequent steps similar to the first embodiment shown in FIG. structure shown.
以下将说明本实施例的效果和优点。Effects and advantages of this embodiment will be described below.
复合缺陷D2b,类似于第一实施例中的p型衬底PSB1中的注入引发的缺陷D2a,具有结束载流子寿命的作用,以允许在p型衬底PSB1中的通过光电转换而产生的电子迅速消失。因此重掺杂p型外延层PE1a的存在可以抑制由p型衬底PSB1中的电子造成的电子串扰或模糊现象的产生。The recombination defect D2b, similar to the implantation-induced defect D2a in the p-type substrate PSB1 in the first embodiment, has the effect of ending the lifetime of carriers to allow the generation of photoelectric conversion in the p-type substrate PSB1 Electrons disappear quickly. Therefore, the existence of the heavily doped p-type epitaxial layer PE1a can suppress the occurrence of electronic crosstalk or blur caused by electrons in the p-type substrate PSB1.
重掺杂p型外延层PE1a还可以作为氧扩散阻挡层。具体来说,重掺杂p型外延层PE1a具有抑制p型衬底PSB1中的氧以及例如来源于其的微小缺陷D1在第二p型外延层PE2的方向上的扩散的功能。这使得其能够抑制扩展缺陷进入第二p型外延层PE2,并且因此抑制由于复合而造成的第二p型外延层PE2中电子的消失(电子寿命的减少)。因此,光电二极管PD1具有增强的灵敏度。The heavily doped p-type epitaxial layer PE1a can also serve as an oxygen diffusion barrier layer. Specifically, the heavily doped p-type epitaxial layer PE1a has the function of suppressing the diffusion of oxygen in the p-type substrate PSB1 and, for example, tiny defects D1 derived therefrom in the direction of the second p-type epitaxial layer PE2. This makes it possible to suppress the entry of extended defects into the second p-type epitaxial layer PE2, and thus suppress the disappearance of electrons in the second p-type epitaxial layer PE2 due to recombination (reduction in electron lifetime). Therefore, the photodiode PD1 has enhanced sensitivity.
在本实施例中,仅通过热处理形成复合缺陷D2b,而不是第一实施例中通过离子注入技术形成注入引发的缺陷D2a。省略采用用于形成扩展缺陷的离子注入技术的步骤可以致使成本降低。In this embodiment, the composite defect D2b is formed only by heat treatment, instead of the implantation-induced defect D2a formed by the ion implantation technique in the first embodiment. Omitting the step of employing ion implantation techniques for forming extended defects can result in cost reduction.
如上所述,在构成第一p型外延层PE1的层中,重掺杂p型外延层PE1a形成为具有高于其它p型外延层PE1b和PE1c的氧浓度,这归因于p型衬底PSB1中包含的氧(包括微小缺陷D1)扩散进入作为最接近p型衬底PSB1的衬底邻近层的重掺杂p型外延层PE1a。重掺杂p型外延层PE1a的氧浓度高于其他p型外延层的氧浓度会提高重掺杂p型外延层PE1a中的复合缺陷D2的形成效率,并且增强重掺杂p型外延层PE1a作为势垒的功能。As described above, among the layers constituting the first p-type epitaxial layer PE1, the heavily doped p-type epitaxial layer PE1a is formed to have a higher oxygen concentration than the other p-type epitaxial layers PE1b and PE1c due to the p-type substrate Oxygen contained in PSB1 (including microdefects D1 ) diffuses into heavily doped p-type epitaxial layer PE1 a which is a substrate-adjacent layer closest to p-type substrate PSB1 . The oxygen concentration of the heavily doped p-type epitaxial layer PE1a is higher than that of other p-type epitaxial layers will increase the formation efficiency of the composite defect D2 in the heavily doped p-type epitaxial layer PE1a, and enhance the formation efficiency of the heavily doped p-type epitaxial layer PE1a function as a barrier.
(第三实施例)(third embodiment)
参考图22,以下将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD的构造以及包括光电二极管PD的转移晶体管TMI。Referring to FIG. 22 , the configuration of the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described in detail below.
图22是示出与图4中所示的第一实施例相同的区域的模式的示意截面图。如图22所示,具有高于图16中的p型衬底PSB1的p型杂质浓度的p型衬底PSB2用作半导体衬底SUB。更具体地,p型衬底PSB2的p型杂质浓度等于构成第一p型外延层PE1的重掺杂p型外延层PE1c的p型杂质浓度。而且,第一p型外延层PE1的p型杂质浓度等于第一和第二实施例的p型外延层PE1的p型杂质浓度。在本实施例中,p型衬底PSB2的p型杂质浓度远高于第二p型外延层PE2的p型杂质浓度。Fig. 22 is a schematic cross-sectional view showing a pattern of the same region as that of the first embodiment shown in Fig. 4 . As shown in FIG. 22, a p-type substrate PSB2 having a higher p-type impurity concentration than p-type substrate PSB1 in FIG. 16 is used as a semiconductor substrate SUB. More specifically, the p-type impurity concentration of the p-type substrate PSB2 is equal to the p-type impurity concentration of the heavily doped p-type epitaxial layer PE1c constituting the first p-type epitaxial layer PE1. Also, the p-type impurity concentration of the first p-type epitaxial layer PE1 is equal to the p-type impurity concentration of the p-type epitaxial layer PE1 of the first and second embodiments. In this embodiment, the p-type impurity concentration of the p-type substrate PSB2 is much higher than the p-type impurity concentration of the second p-type epitaxial layer PE2.
p型衬底PSB2中包含微小缺陷D1和复合缺陷D2b。由于在p型衬底PSB2中,例如p型衬底PSB2中的硼的p型杂质和扩散进入p型衬底PSB2中的氧沉淀核(例如构成微小缺陷D1的那些)之间的反应而形成复合缺陷D2b。The p-type substrate PSB2 contains tiny defects D1 and composite defects D2b. Formed due to a reaction between p-type impurities such as boron in the p-type substrate PSB2 and oxygen precipitation nuclei (such as those constituting minute defects D1) diffused into the p-type substrate PSB2 in the p-type substrate PSB2 Compound Defect D2b.
p型衬底PSB2的主表面上的第一p型外延层PE1包括彼此不同的多个p型外延层,并且其从p型衬底PSB2一侧依次具有堆叠的轻掺杂p型外延层PE1b以及重掺杂p型外延层PE1c。它们类似于第二实施例。The first p-type epitaxial layer PE1 on the main surface of the p-type substrate PSB2 includes a plurality of p-type epitaxial layers different from each other, and it has stacked lightly doped p-type epitaxial layers PE1b sequentially from the side of the p-type substrate PSB2 And heavily doped p-type epitaxial layer PE1c. They are similar to the second embodiment.
这意味着在本实施例中,其中形成复合缺陷D2b的第二实施例的重掺杂p型外延层PE1a与p型衬底PSB2成一体。因此p型衬底PSB2的p型杂质浓度高,这是因为重掺杂p型外延层PE1a的高p型杂质浓度。This means that in this embodiment, the heavily doped p-type epitaxial layer PE1a of the second embodiment in which the composite defect D2b is formed is integrated with the p-type substrate PSB2. The p-type impurity concentration of the p-type substrate PSB2 is therefore high because of the high p-type impurity concentration of the heavily doped p-type epitaxial layer PE1a.
除上述外延层之外,本实施例的构造基本上类似于图16中所示的第二实施例,因此相同的部件由相同的参考符号表示,并且省略重复说明。Except for the above-described epitaxial layer, the configuration of this embodiment is basically similar to that of the second embodiment shown in FIG. 16 , so the same components are denoted by the same reference symbols, and repeated explanations are omitted.
参考图23至26,将说明制造构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移晶体管TMI的方法。图23至26示出与图22相同的区域的处理。Referring to FIGS. 23 to 26 , a method of manufacturing the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described. 23 to 26 show processing of the same area as FIG. 22 .
如图23所示,p型衬底PSB2提供作为例如由硅制成的p型衬底。p型衬底PSB2中的诸如硼的p型杂质的浓度设定为4E17cm-3以上但不大于1E20cm-3,其例如高于第一实施例的p型衬底PSB1的p型杂质浓度。通过一般公知的方法热处理p型衬底PSB2以在p型衬底PSB2中形成作为例如用于形成BMD的微小缺陷核Dc1的氧。As shown in FIG. 23, a p-type substrate PSB2 is provided as a p-type substrate made of, for example, silicon. The concentration of p-type impurities such as boron in p-type substrate PSB2 is set to 4E17 cm -3 or more but not more than 1E20 cm -3 , which is higher than that of p-type substrate PSB1 of the first embodiment, for example. The p-type substrate PSB2 is heat-treated by a generally known method to form oxygen in the p-type substrate PSB2 as, for example, minute defect nuclei Dc1 for forming BMD.
如图24所示,通过在p型衬底PSB2的主表面上通过典型地外延生长形成由多个层构成的第一p型外延层PE1。本文所用的术语“多个层”例如是指通过从靠近p型衬底PSB2一侧依次堆叠轻掺杂p型外延层PE1b以及重掺杂p型外延层PE1c而形成的两层。重掺杂p型外延层PE1c包含作为p型杂质的硼,其浓度等于第一实施例的第一p型外延层PE1中硼的浓度。优选将硼的浓度设定为例如4E17cm-3以上但不大于1E20cm-3。轻掺杂p型外延层PE1b包含作为p型杂质的硼,其浓度等于第一实施例的第二p型外延层PE2中硼的浓度。优选硼的浓度例如设定为5E14cm-3以上但不大于1E16cm-3。通过热处理,可以将微小缺陷核Dc1生长成微小缺陷D1。As shown in FIG. 24, the first p-type epitaxial layer PE1 composed of a plurality of layers is formed by typically epitaxial growth on the main surface of the p-type substrate PSB2. The term "plurality of layers" used herein refers to, for example, two layers formed by sequentially stacking a lightly doped p-type epitaxial layer PE1b and a heavily doped p-type epitaxial layer PE1c from the side close to the p-type substrate PSB2. The heavily doped p-type epitaxial layer PE1c contains boron as a p-type impurity at a concentration equal to that of boron in the first p-type epitaxial layer PE1 of the first embodiment. The concentration of boron is preferably set to, for example, 4E17 cm -3 or more but not more than 1E20 cm -3 . The lightly doped p-type epitaxial layer PE1b contains boron as a p-type impurity at a concentration equal to that of boron in the second p-type epitaxial layer PE2 of the first embodiment. The concentration of boron is preferably set to, for example, 5E14 cm -3 or more but not more than 1E16 cm -3 . By heat treatment, the minute defect core Dc1 can be grown into a minute defect D1.
如图25所示,对图24中形成的结构进行热处理。通过这种热处理,p型衬底PSB2中包含的氧(包括微小缺陷D1)扩散并与p型衬底PSB2中的p型杂质的硼反应,从而在p型衬底PSB2中形成复合缺陷D2b。As shown in FIG. 25, the structure formed in FIG. 24 is subjected to heat treatment. Through this heat treatment, oxygen contained in p-type substrate PSB2 (including minute defects D1) diffuses and reacts with boron as a p-type impurity in p-type substrate PSB2, thereby forming complex defects D2b in p-type substrate PSB2.
如图26所示,形成由硅制成的第二p型外延层PE2,以便覆盖第一p型外延层PE1c的上表面。第二p型外延层PE2例如也包含作为p型杂质的硼。优选例如将硼的浓度设定为5E14cm-3以上但不大于1E16cm-3。因此,在本实施例中,p型杂质形成在p型衬底PSB2中,以便p型衬底PSB2中的p型杂质浓度高于第二p型外延层PE2中的p型杂质浓度。随后,执行类似于图8至10中所示的第一实施例的处理,之后执行类似于图10中所示的第一实施例的后续步骤,从而形成图22中所示的结构。As shown in FIG. 26, the second p-type epitaxial layer PE2 made of silicon is formed so as to cover the upper surface of the first p-type epitaxial layer PE1c. The second p-type epitaxial layer PE2 also contains, for example, boron as a p-type impurity. It is preferable to set the concentration of boron, for example, to 5E14 cm -3 or more but not more than 1E16 cm -3 . Therefore, in the present embodiment, p-type impurities are formed in p-type substrate PSB2 so that the p-type impurity concentration in p-type substrate PSB2 is higher than the p-type impurity concentration in second p-type epitaxial layer PE2. Subsequently, processing similar to that of the first embodiment shown in FIGS. 8 to 10 is performed, followed by subsequent steps similar to that of the first embodiment shown in FIG. 10 , thereby forming the structure shown in FIG. 22 .
以下将说明本实施例的效果和优点。除类似于第二实施例的效果和优点之外,本实施例还具有如下效果和优点。Effects and advantages of this embodiment will be described below. In addition to the effects and advantages similar to those of the second embodiment, this embodiment has the following effects and advantages.
在本实施例中,p型衬底PSB2中的p型杂质浓度设定为远高于第二p型外延层PE2的杂质浓度。更具体地,p型衬底PSB2中的p型杂质浓度与第二实施例中的重掺杂p型外延层PE1a的杂质浓度一样高。因此第二实施例中的重掺杂p型外延层PE1a与半导体衬底(p型衬底PSB2)成一体。这使得其能省略形成重掺杂p型外延层PE1a的步骤,致使步骤数量的减少和成本降低。In this embodiment, the p-type impurity concentration in the p-type substrate PSB2 is set to be much higher than the impurity concentration of the second p-type epitaxial layer PE2. More specifically, the p-type impurity concentration in the p-type substrate PSB2 is as high as that of the heavily doped p-type epitaxial layer PE1a in the second embodiment. The heavily doped p-type epitaxial layer PE1a in the second embodiment is thus integrated with the semiconductor substrate (p-type substrate PSB2). This makes it possible to omit the step of forming the heavily doped p-type epitaxial layer PE1a, resulting in a reduction in the number of steps and a reduction in cost.
在本实施例中,因为p型衬底PSB2的p型杂质浓度高,因此可以增强p型衬底PSB2中的p型杂质和p型衬底PSB2中的氧(包括微小缺陷核Dc1)之间的反应性,这对在p型衬底PSB2中形成复合缺陷D2b高度有效。由于p型衬底PSB2中富集丰富的复合缺陷D2b,因此可以减少p型衬底PSB2中电子的载流子寿命。In this embodiment, since the p-type impurity concentration of the p-type substrate PSB2 is high, the relationship between the p-type impurities in the p-type substrate PSB2 and the oxygen (including the tiny defect core Dc1) in the p-type substrate PSB2 can be enhanced. , which is highly effective for forming recombination defect D2b in p-type substrate PSB2. Since the p-type substrate PSB2 is rich in recombination defects D2b, the carrier lifetime of electrons in the p-type substrate PSB2 can be reduced.
(第四实施例)(fourth embodiment)
参考图27,以下将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD和包括光电二极管PD的转移晶体管TMI的构造。Referring to FIG. 27 , the configurations of the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described in detail below.
图27是示出与图4中所示的第一实施例相同的区域的模式的示意截面图。如图27所示,来源于引入p型衬底PSB1的诸如氩或硅的杂质元素的多个扩展缺陷D2a构成p型衬底PSB1中的掩埋层BRD。FIG. 27 is a schematic cross-sectional view showing a pattern of the same region as that of the first embodiment shown in FIG. 4 . As shown in FIG. 27, a plurality of extended defects D2a originating from an impurity element such as argon or silicon introduced into the p-type substrate PSB1 constitutes the buried layer BRD in the p-type substrate PSB1.
掩埋层BRD位于深于p型衬底PSB1的主表面的区域中,并且掩埋层BRD没有邻接p型衬底PSB1的主表面。因为掩埋层BRD包含用于形成扩展缺陷D2a的大量杂质元素,因此掩埋层的p型杂质浓度高于除掩埋层BRD之外的p型衬底PSB1的部分的杂质浓度。The buried layer BRD is located in a region deeper than the main surface of the p-type substrate PSB1, and the buried layer BRD does not adjoin the main surface of the p-type substrate PSB1. Since the buried layer BRD contains a large amount of impurity elements for forming the extended defect D2a, the p-type impurity concentration of the buried layer is higher than that of the portion of the p-type substrate PSB1 other than the buried layer BRD.
虽然掩埋层BRD位于p型衬底PSB1中,但是从p型杂质浓度的观点来看,其例如类似于第二实施例的重掺杂p型外延层PE1a。因为类似于图27中的掩埋层BRD下方的p型衬底PSB1的区域,掩埋层BRD上方的区域(第二p型外延层PE2的一侧上)是低p型杂质浓度区,因此从p型杂质浓度的观点来看,其例如类似于第二实施例的轻掺杂p型外延层PE1b。p型衬底PSB1在其主表面上具有类似于第二实施例的重掺杂p型外延层PE1c的单层。Although the buried layer BRD is located in the p-type substrate PSB1, it is, for example, similar to the heavily doped p-type epitaxial layer PE1a of the second embodiment from the viewpoint of p-type impurity concentration. Because the region above the buried layer BRD (on the side of the second p-type epitaxial layer PE2) is a low p-type impurity concentration region similar to the region of the p-type substrate PSB1 below the buried layer BRD in FIG. From the viewpoint of the p-type impurity concentration, it is, for example, similar to the lightly doped p-type epitaxial layer PE1b of the second embodiment. The p-type substrate PSB1 has on its main surface a single layer similar to the heavily doped p-type epitaxial layer PE1c of the second embodiment.
假设第二实施例的重掺杂p型外延层PE1a和轻掺杂p型外延层PE1b与本实施例中的p型衬底PSB1成一体。It is assumed that the heavily doped p-type epitaxial layer PE1a and the lightly doped p-type epitaxial layer PE1b of the second embodiment are integrated with the p-type substrate PSB1 in this embodiment.
掩埋层BRD是由形成在p型衬底PSB1中的注入引发的缺陷D2a形成的区域,因此本实施例的构造完全类似于图4中所示的在p型衬底PSB1中具有扩展缺陷D2a(两个以上)的第一实施例的构造。这意味着在本实施例中,从不同于图4的观点,同时关注p型衬底PSB1中的其内具有注入引发的缺陷D2a的重掺杂区域(掩埋层BRD)和重掺杂区域正上方的轻掺杂区域来说明图4中所示的第一实施例的构造。The buried layer BRD is a region formed by implantation-induced defects D2a formed in the p-type substrate PSB1, so the configuration of this embodiment is completely similar to that shown in FIG. 4 with extended defects D2a in the p-type substrate PSB1 ( Two or more) of the construction of the first embodiment. This means that in the present embodiment, from a viewpoint different from FIG. The upper lightly doped region is used to illustrate the construction of the first embodiment shown in FIG. 4 .
除上述一点之外,本实施例的构造基本上类似于图4中所示的第一实施例的构造,因此相同的部件由相同的参考数字表示并且省略重复说明。Except for the above point, the configuration of the present embodiment is basically similar to that of the first embodiment shown in FIG. 4 , and thus the same components are denoted by the same reference numerals and repeated explanations are omitted.
参考图28和29,将说明制造构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD和包括光电二极管PD的转移晶体管TMI的方法。图28和29示出与图27相同的区域的处理。Referring to FIGS. 28 and 29 , a method of manufacturing the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described. 28 and 29 show processing of the same area as in FIG. 27 .
如图28所示,在图5的步骤中提供p型衬底PSB1之后,通过采用典型的离子注入技术在衬底中(略深于p型衬底PSB1的主表面S1的区域)形成例如硼的杂质元素。以一般公知方式对p型衬底PSB1进行热处理。随后,由于引入作为杂质元素的硼,因此在衬底中掩埋了诸如位错环的扩展缺陷D2a。而且通过这种热处理,将p型衬底PSB1中的氧生长成微小缺陷D1。As shown in FIG. 28, after the p-type substrate PSB1 is provided in the step of FIG. impurity elements. The p-type substrate PSB1 is thermally treated in a generally known manner. Subsequently, due to the introduction of boron as an impurity element, extended defects D2a such as dislocation loops are buried in the substrate. And by this heat treatment, the oxygen in the p-type substrate PSB1 grows into minute defects D1.
如图29所示,通过典型的外延生长在p型衬底PSB1的主表面S1上形成由硅制成的第一p型外延层PE1(类似于第二实施例的重掺杂p型外延层PE1c)。As shown in FIG. 29, a first p-type epitaxial layer PE1 made of silicon (similar to the heavily doped p-type epitaxial layer of the second embodiment) is formed on the main surface S1 of the p-type substrate PSB1 by typical epitaxial growth. PE1c).
执行类似于图8至10中所示的第一实施例的处理,随后执行类似于图10中所示的第一实施例的后续步骤以形成图27中所示的结构。Processing similar to that of the first embodiment shown in FIGS. 8 to 10 is performed, followed by subsequent steps similar to that of the first embodiment shown in FIG. 10 to form the structure shown in FIG. 27 .
随后将说明本实施例的效果和优点。除类似于第二实施例的效果和优点之外,本实施例还展现以下效果和优点。Effects and advantages of this embodiment will be described later. In addition to the effects and advantages similar to the second embodiment, this embodiment exhibits the following effects and advantages.
在本实施例中,第二实施例中的重掺杂p型外延层PE1a和轻掺杂p型外延层PE1b与半导体衬底(p型衬底PSB1)成一体。这使得其能够省略形成重掺杂p型外延层PE1a和轻掺杂p型外延层PE1b的步骤,致使步骤数量的减少以及成本降低。In this embodiment, the heavily doped p-type epitaxial layer PE1a and the lightly doped p-type epitaxial layer PE1b in the second embodiment are integrated with the semiconductor substrate (p-type substrate PSB1). This makes it possible to omit the step of forming the heavily doped p-type epitaxial layer PE1a and the lightly doped p-type epitaxial layer PE1b, resulting in a reduction in the number of steps and a reduction in cost.
(第五实施例)(fifth embodiment)
参考图30,以下将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移晶体管TMI的构造。Referring to FIG. 30 , the configurations of the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described in detail below.
图30是示出与第一实施例中的图4相同的区域的模式的示意截面图。如图30所示,本实施例采用n型衬底NSB替代p型衬底PSB1。这意味着n型衬底NSB具有引入其中的诸如锑,砷或磷的n型杂质元素。Fig. 30 is a schematic cross-sectional view showing a pattern of the same area as Fig. 4 in the first embodiment. As shown in FIG. 30 , in this embodiment, an n-type substrate NSB is used instead of a p-type substrate PSB1 . This means that the n-type substrate NSB has n-type impurity elements such as antimony, arsenic or phosphorus introduced therein.
除上述衬底之外,本实施例的构造基本上类似于图4中所示的第一实施例,因此相同的部件由相同的参考数字表示并且省略重复说明。Except for the substrate described above, the configuration of this embodiment is basically similar to that of the first embodiment shown in FIG. 4, so the same components are denoted by the same reference numerals and repeated descriptions are omitted.
本实施例采用n型衬底NSB替代p型衬底PSB1或PSB2,因此在n型衬底NSB中,能以高比率收集在n型衬底NSB中通过长波长光的光电转换而产生的电子。因此能抑制串扰,即已经通过光电转换而产生的电子的被与接收长波长光的光电二极管PD1相邻的光电二极管PD2不期望地收集的发生。In this embodiment, the n-type substrate NSB is used instead of the p-type substrate PSB1 or PSB2, so in the n-type substrate NSB, electrons generated by photoelectric conversion of long-wavelength light in the n-type substrate NSB can be collected at a high rate . It is therefore possible to suppress crosstalk, that is, the occurrence of electrons that have been generated through photoelectric conversion being undesirably collected by the photodiode PD2 adjacent to the photodiode PD1 that receives long-wavelength light.
(第六实施例)(sixth embodiment)
参考图31,以下将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD的构造以及包括光电二极管PD的转移晶体管TMI。Referring to FIG. 31 , the configuration of the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described in detail below.
图31是示出与图4中所示的第一实施例相同的区域的模式的示意截面图。如图31所示,本实施例具有n型衬底NSB正下方的背电极EE。通过在n型衬底NSB的下侧上的主表面上沉积诸如金的金属材料薄膜而获得背电极EE。Fig. 31 is a schematic cross-sectional view showing a pattern of the same region as that of the first embodiment shown in Fig. 4 . As shown in FIG. 31 , this embodiment has a back electrode EE directly under the n-type substrate NSB. The back electrode EE is obtained by depositing a thin film of metallic material such as gold on the main surface on the underside of the n-type substrate NSB.
除上述背电极之外,本实施例的构造基本上类似于图30中所示的第五实施例,因此相同的部件由相同的参考数字表示并且省略重复说明。Except for the above-mentioned back electrode, the configuration of this embodiment is basically similar to that of the fifth embodiment shown in FIG. 30 , and thus the same components are denoted by the same reference numerals and repeated explanations are omitted.
在图30中所示的第五实施例的构造中,当由于特别地有源光电转换而在n型衬底NSB中产生大量电子,并且此外n型衬底NSB中的电子具有长寿命时,n型衬底NSB中的某些电子例如会穿透第一注入区PJ1。这种现象的发生是由于n型衬底NSB不能允许电子从其溢出,且所谓的浮置状态发生在n型衬底NSB中。电子穿透进入第一注入区PJ1会导致由电子造成的串扰。In the configuration of the fifth embodiment shown in FIG. 30, when a large amount of electrons are generated in the n-type substrate NSB due to particularly active photoelectric conversion, and furthermore the electrons in the n-type substrate NSB have a long lifetime, Some electrons in the n-type substrate NSB, for example, will penetrate through the first injection region PJ1. This phenomenon occurs because the n-type substrate NSB cannot allow electrons to overflow therefrom, and a so-called floating state occurs in the n-type substrate NSB. Penetration of electrons into the first injection region PJ1 results in crosstalk caused by electrons.
如图31中所示,通过在n型衬底NSB正下方形成背电极EE并将接地电势GND施加至背电极EE,以固定n型衬底NSB的电势,因此n型衬底NSB中产生的过量电子能从背电极EE引入接地电势GND一侧。这会降低n型衬底NSB中过量电子造成串扰的可能性。As shown in FIG. 31, the potential of the n-type substrate NSB is fixed by forming the back electrode EE directly under the n-type substrate NSB and applying the ground potential GND to the back electrode EE, so that the potential generated in the n-type substrate NSB Excess electrons can be introduced from the back electrode EE to the ground potential GND side. This reduces the possibility of crosstalk from excess electrons in the n-type substrate NSB.
(第七实施例)(seventh embodiment)
参考图32,以下将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移晶体管TMI的构造。Referring to FIG. 32 , the configurations of the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described in detail below.
图32是示出与图4中所示的第一实施例相同的区域的模式的示意截面图。如图32所示,本实施例具有基本上类似于图4中所示的第一实施例的构造,但是本实施例与第一实施例的不同点如下。Fig. 32 is a schematic cross-sectional view showing a pattern of the same region as that of the first embodiment shown in Fig. 4 . As shown in FIG. 32, the present embodiment has a configuration basically similar to that of the first embodiment shown in FIG. 4, but the present embodiment differs from the first embodiment in the following points.
具体来说,如图32所示,本实施例不具有图4中形成的第一注入区PJ1但是具有第二外延层PE2,以便覆盖光电二极管PD1和光电二极管PD2下方的第一p型外延层PE1的上表面。第一像素区RPx中的第二p型外延层PE2的厚度基本上等于第二像素区GPx中的第二p型外延层PE2的厚度。此外,第二注入区PJ2到达第一p型外延层PE1,并且其与第一p型外延层PE1接触。Specifically, as shown in FIG. 32, this embodiment does not have the first implantation region PJ1 formed in FIG. 4 but has a second epitaxial layer PE2 so as to cover the photodiode PD1 and the first p-type epitaxial layer below the photodiode PD2. The upper surface of PE1. The thickness of the second p-type epitaxial layer PE2 in the first pixel region RPx is substantially equal to the thickness of the second p-type epitaxial layer PE2 in the second pixel region GPx. In addition, the second implantation region PJ2 reaches the first p-type epitaxial layer PE1, and it is in contact with the first p-type epitaxial layer PE1.
图32中所示的第二p型外延层PE2优选薄于图4中所示的第二p型外延层PE2。例如,图32中的第二p型外延层PE2的厚度优选基本上等于图4中的第二像素区GPx中的第二p型外延层PE2的厚度(除第一注入区PJ1之外)。The second p-type epitaxial layer PE2 shown in FIG. 32 is preferably thinner than the second p-type epitaxial layer PE2 shown in FIG. 4 . For example, the thickness of the second p-type epitaxial layer PE2 in FIG. 32 is preferably substantially equal to the thickness of the second p-type epitaxial layer PE2 in the second pixel region GPx in FIG. 4 (except for the first injection region PJ1 ).
除上述要点之外,本实施例的构造基本上类似于图4中所示的第一实施例,因此相同的部件由相同的参考数字表示并且省略重复说明。Except for the above points, the configuration of this embodiment is basically similar to that of the first embodiment shown in FIG. 4 , and thus the same components are denoted by the same reference numerals and repeated explanations are omitted.
参考图33,以下将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD的构造以及包括光电二极管PD的转移晶体管TMI。在图33中示出类似于图32的区域的处理。Referring to FIG. 33 , the configuration of the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described in detail below. Processing of an area similar to that of FIG. 32 is shown in FIG. 33 .
如图33所示,在类似于图5至7中所示的第一实施例的处理之后,形成第二p型外延层PE2以便覆盖光电二极管PD1的形成区和光电二极管PD2的形成区下方的第一p型外延层PE1的上表面。换言之,形成第二p型外延层PE2以便覆盖第一像素区RPx的形成区和第二像素区GPx的形成区中的第一p型外延层PE1的上表面。As shown in FIG. 33, after a process similar to that of the first embodiment shown in FIGS. 5 to 7, the second p-type epitaxial layer PE2 is formed so as to cover the formation region of the photodiode PD1 and the area below the formation region of the photodiode PD2. the upper surface of the first p-type epitaxial layer PE1. In other words, the second p-type epitaxial layer PE2 is formed so as to cover the upper surface of the first p-type epitaxial layer PE1 in the formation region of the first pixel region RPx and the formation region of the second pixel region GPx.
在本实施例中,第二p型外延层PE2的厚度优选小于例如图8的步骤形成的第二p型外延层PE2。In this embodiment, the thickness of the second p-type epitaxial layer PE2 is preferably smaller than, for example, the second p-type epitaxial layer PE2 formed by the steps in FIG. 8 .
在形成第二p型外延层之后,执行类似于图8至10中所示的第一实施例的那些的处理,并且随后执行类似于图10中所示的第一实施例的后续步骤,以形成图32中所示的结构。After forming the second p-type epitaxial layer, processes similar to those of the first embodiment shown in FIGS. 8 to 10 are performed, and then subsequent steps similar to those of the first embodiment shown in FIG. 10 are performed to The structure shown in Figure 32 is formed.
本实施例不具有第一注入区PJ1,因此可以减少将要提供的掩膜数量,制造间歇时间以及制造成本。This embodiment does not have the first implantation region PJ1, so the number of masks to be provided, the manufacturing tact time, and the manufacturing cost can be reduced.
(第八实施例)(eighth embodiment)
参考图34,以下将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD的构造以及包括光电二极管PD的转移晶体管TMI。Referring to FIG. 34 , the configuration of the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described in detail below.
图34是示出与图4中所示的第一实施例相同的区域的模式的示意截面图。如图34所示,本实施例具有类似于图32中所示的第七实施例的构造,但是在形成第二注入区PJ2时由离子注入技术提供的能量要高于图32的情况。Fig. 34 is a schematic cross-sectional view showing a pattern of the same region as that of the first embodiment shown in Fig. 4 . As shown in FIG. 34, this embodiment has a configuration similar to that of the seventh embodiment shown in FIG. 32, but the energy provided by the ion implantation technique in forming the second implantation region PJ2 is higher than that of the case of FIG.
与图32的第二注入区PJ2相比,增大能量可以增强作为势垒用于抑制第二p型外延层PE2中已经通过光电转换而产生的电子在第一像素区RPx和第二像素区GPx之间的迁移的图34的第二注入区PJ2的功能。Compared with the second injection region PJ2 in FIG. 32 , increasing the energy can enhance the potential barrier used to suppress electrons generated through photoelectric conversion in the second p-type epitaxial layer PE2 in the first pixel region RPx and the second pixel region. The function of the second implanted region PJ2 of Figure 34 for migration between GPx.
可以使图34中的第二p型外延层PE2的厚度大于图32中的情况。因为本实施例中用于形成第二注入区PJ2的能量高于第七实施例中的情况,因此本实施例中的第二注入区PJ2可以具有比第七实施例的深度更大的深度。即使通过形成第二注入区PJ2以便与第一p型外延层PE1接触而将第二p型外延层PE2的厚度制造得更大,也能增强抑制第二像素区GPx中的第二p型外延层PE2中电子串扰的效果。因为可以将第二p型外延层PE2的厚度制造得更大,因此可以扩展通过光电二极管PD1收集的光电转换电子的生成区域,使得其能够改善光电二极管PD1的灵敏度。The thickness of the second p-type epitaxial layer PE2 in FIG. 34 can be made larger than that in FIG. 32 . Since the energy used to form the second implantation region PJ2 in this embodiment is higher than that in the seventh embodiment, the second implantation region PJ2 in this embodiment may have a greater depth than that in the seventh embodiment. Even if the thickness of the second p-type epitaxial layer PE2 is made larger by forming the second implantation region PJ2 so as to be in contact with the first p-type epitaxial layer PE1, the suppression of the second p-type epitaxial layer in the second pixel region GPx can be enhanced. Effect of electron crosstalk in layer PE2. Since the thickness of the second p-type epitaxial layer PE2 can be made larger, the generation area of photoelectric conversion electrons collected by the photodiode PD1 can be expanded, making it possible to improve the sensitivity of the photodiode PD1.
(第九实施例)(ninth embodiment)
参考图35,以下将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移晶体管TMI的构造。Referring to FIG. 35 , the configurations of the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described in detail below.
图35是示出与图4中所示的第一实施例相同的区域的模式的示意截面图。如图35所示,本实施例具有位于第一像素区RPx和第二像素区GPx之间的边界部处在沟槽隔离TI下方的像素隔离区SPT。像素隔离区SPT由深沟槽DT和第三p型外延层PE3构成。Fig. 35 is a schematic cross-sectional view showing a pattern of the same region as that of the first embodiment shown in Fig. 4 . As shown in FIG. 35 , the present embodiment has a pixel isolation region SPT located below the trench isolation TI at the boundary portion between the first pixel region RPx and the second pixel region GPx. The pixel isolation region SPT is composed of a deep trench DT and a third p-type epitaxial layer PE3.
深沟槽DT是穿透第二外延层PE2并到达第一像素区RPx和第二像素区GPx之间边界部的第一p型外延层PE1的沟槽。深沟槽DT优选与沟槽隔离TI的最下部接触。The deep trench DT is a trench of the first p-type epitaxial layer PE1 that penetrates the second epitaxial layer PE2 and reaches the boundary portion between the first pixel region RPx and the second pixel region GPx. The deep trench DT is preferably in contact with the lowermost portion of the trench isolation TI.
深沟槽DT在其中具有作为p型半导体层的第三p型外延层PE3。换言之,深沟槽DT由作为p型半导体层的第三p型外延层PE3填充。在上述各个实施例中,第三p型外延层PE3都对应于作为第二p型杂质区的第二注入区PJ2,并且功能类似于第二注入区PJ2。The deep trench DT has therein the third p-type epitaxial layer PE3 as a p-type semiconductor layer. In other words, deep trench DT is filled with third p-type epitaxial layer PE3 as a p-type semiconductor layer. In each of the above embodiments, the third p-type epitaxial layer PE3 corresponds to the second implantation region PJ2 as the second p-type impurity region, and has a function similar to that of the second implantation region PJ2.
类似于第七或第八实施例,本实施例不具有第二像素区GPx中的第一注入区PJ1。Similar to the seventh or eighth embodiment, this embodiment does not have the first injection region PJ1 in the second pixel region GPx.
除上述要点之外,本实施例的构造基本上类似于图4中所示的第一实施例,因此相同的部件由相同的参考符号表示并且省略其说明。Except for the above points, the configuration of this embodiment is basically similar to that of the first embodiment shown in FIG. 4 , so the same components are denoted by the same reference symbols and their descriptions are omitted.
参考图36至38,以下将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移晶体管TMI的构造。Referring to FIGS. 36 to 38 , the configurations of the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described in detail below.
如图36所示,在类似于图5至7中所示的第一实施例的那些处理之后,在类似于图8的步骤中形成第二p型外延层PE2。随后,通过采用典型的光刻和蚀刻在第一像素区RPx的形成区和第二像素区GPx的形成区之间的边界部处的第二p型外延层PE2中形成穿透第二p型外延层PE2以便到达第一p型外延层PE1的深沟槽DT。As shown in FIG. 36 , after processes similar to those of the first embodiment shown in FIGS. 5 to 7 , the second p-type epitaxial layer PE2 is formed in a step similar to that of FIG. 8 . Subsequently, a penetrating second p-type epitaxial layer PE2 is formed in the boundary portion between the formation region of the first pixel region RPx and the formation region of the second pixel region GPx by employing typical photolithography and etching. The epitaxial layer PE2 so as to reach the deep trench DT of the first p-type epitaxial layer PE1.
如图37所示,通过典型的外延生长,第三p型外延层PE3形成在第二p型外延层PE2的上表面上以填充深沟槽DT。As shown in FIG. 37 , by typical epitaxial growth, a third p-type epitaxial layer PE3 is formed on the upper surface of the second p-type epitaxial layer PE2 to fill the deep trench DT.
如图38所示,利用被称为CMP的化学机械抛光移除第二p型外延层PE2上的第三p型外延层PE3。因此,在第一像素区RPx的形成区和第二像素区GPx的形成区之间的边界部处形成像素隔离区SPT。随后通过典型的光刻和蚀刻在第二p型外延层PE2中的像素隔离区SPT的正上方形成浅沟槽。随后,例如通过采用典型的CVD将诸如氧化硅膜的绝缘膜形成在第二p型外延层PE2的上表面上,从而填充浅沟槽。As shown in FIG. 38 , the third p-type epitaxial layer PE3 on the second p-type epitaxial layer PE2 is removed by chemical mechanical polishing called CMP. Accordingly, the pixel isolation region SPT is formed at a boundary portion between the formation region of the first pixel region RPx and the formation region of the second pixel region GPx. A shallow trench is then formed directly above the pixel isolation region SPT in the second p-type epitaxial layer PE2 by typical photolithography and etching. Subsequently, an insulating film such as a silicon oxide film is formed on the upper surface of the second p-type epitaxial layer PE2 by, for example, typical CVD, thereby filling the shallow trench.
随后,再次通过采用CMP移除第二p型外延层PE2上的绝缘膜以在像素隔离区SPT正上方形成沟槽隔离TI。Subsequently, the insulating film on the second p-type epitaxial layer PE2 is removed again by using CMP to form a trench isolation TI right above the pixel isolation region SPT.
随后执行类似于图9和10中所示的第一实施例的那些处理,随后执行类似于第一实施例的图10的后续步骤以形成图35中所示的结构。Subsequently, processes similar to those of the first embodiment shown in FIGS. 9 and 10 are performed, followed by subsequent steps similar to those of FIG. 10 of the first embodiment to form the structure shown in FIG. 35 .
以下将说明本实施例的效果和优点。如本实施例那样,替代第二注入区PJ2,可以通过在深沟槽DT中填充第三p型外延层PE3而在第一像素区RPx和第二像素区GPx之间形成势垒。因为第三p型外延层PE3通过外延生长形成,因此可以自由地形成第三p型外延层PE3,以便具有高于通过离子注入技术形成的第二注入区PJ2的p型杂质浓度。因此像素隔离区SPT变得能更加有效地抑制串扰。Effects and advantages of this embodiment will be described below. Like this embodiment, instead of the second implantation region PJ2, a potential barrier may be formed between the first pixel region RPx and the second pixel region GPx by filling the third p-type epitaxial layer PE3 in the deep trench DT. Since the third p-type epitaxial layer PE3 is formed by epitaxial growth, the third p-type epitaxial layer PE3 can be freely formed so as to have a higher p-type impurity concentration than the second implantation region PJ2 formed by the ion implantation technique. Therefore, the pixel isolation region SPT becomes more effective in suppressing crosstalk.
(第十实施例)(tenth embodiment)
参考图39,以下将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移晶体管TMI的构造。Referring to FIG. 39 , the configurations of the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described in detail below.
图39是示出与图4中所示的第一实施例相同的区域的模式的示意截面图。如图39所示,本实施例具有基本上类似于图35中所示的第九实施例的构造,但是构成像素隔离区SPT的深沟槽DT由第三p型外延层PE3和绝缘膜II填充。Fig. 39 is a schematic cross-sectional view showing a pattern of the same region as that of the first embodiment shown in Fig. 4 . As shown in FIG. 39, the present embodiment has a configuration basically similar to that of the ninth embodiment shown in FIG. filling.
深沟槽DT在其外部由第三外延层PE3填充,并且第三外延层PE3内部的沟槽的部分由绝缘膜II填充。换言之,深沟槽DT中的第三外延层PE3在外延层上具有绝缘膜II。绝缘膜II例如由氧化硅膜制成。这意味着本实施例的像素隔离区SPT包括深沟槽DT、第三p型外延层PE3以及绝缘膜II。The deep trench DT is filled on the outside thereof with the third epitaxial layer PE3, and part of the trench inside the third epitaxial layer PE3 is filled with the insulating film II. In other words, the third epitaxial layer PE3 in the deep trench DT has the insulating film II on the epitaxial layer. The insulating film II is made of, for example, a silicon oxide film. This means that the pixel isolation region SPT of this embodiment includes the deep trench DT, the third p-type epitaxial layer PE3, and the insulating film II.
除上述要点之外,本实施例的构造基本上类似于图35中所示的第九实施例,因此相同的部件由相同的参考数字表示且省略其重复说明。Except for the above points, the configuration of this embodiment is basically similar to that of the ninth embodiment shown in FIG. 35 , so the same components are denoted by the same reference numerals and their repeated descriptions are omitted.
参考图40至42,将说明制造构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移晶体管TMI的方法。Referring to FIGS. 40 to 42 , a method of manufacturing the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described.
如图40所示,在如图36中所示的第九实施例的第二p型外延层PE2中形成深沟槽DT之后,通过采用典型的外延生长在第二p型外延层PE2上形成第三p型外延层PE3,以便覆盖深沟槽DT的内壁。As shown in FIG. 40, after the deep trench DT is formed in the second p-type epitaxial layer PE2 of the ninth embodiment as shown in FIG. The third p-type epitaxial layer PE3 so as to cover the inner wall of the deep trench DT.
如图41所示,通过涂覆形成例如由氧化硅膜制成的绝缘膜II,以便覆盖第二p型外延层PE2上以及深沟槽DT中的第三p型外延层PE3。深沟槽DT由绝缘膜II和第三p型外延层PE3填充。As shown in FIG. 41, an insulating film II made of, for example, a silicon oxide film is formed by coating so as to cover the third p-type epitaxial layer PE3 on the second p-type epitaxial layer PE2 and in the deep trench DT. Deep trench DT is filled with insulating film II and third p-type epitaxial layer PE3.
如图42中所示,利用CMP移除第二p型外延层PE2上的第三p型外延层PE3和绝缘膜II。以此方式,在第一像素区RPx的形成区和第二像素区GPx的形成区之间的边界部处形成像素隔离区SPT。As shown in FIG. 42 , the third p-type epitaxial layer PE3 and the insulating film II on the second p-type epitaxial layer PE2 are removed by CMP. In this way, the pixel isolation region SPT is formed at the boundary portion between the formation region of the first pixel region RPx and the formation region of the second pixel region GPx.
随后执行类似于第九实施例中的像素隔离区SPT的形成之后的那些处理,从而在图像隔离区SPT正上方形成沟槽隔离TI。随后,执行类似于图9至10中所示的第一实施例的那些处理,随后以类似于第一实施例的方式执行图10的后续步骤,从而形成图42中所示的结构。Subsequently, processes similar to those after the formation of the pixel isolation region SPT in the ninth embodiment are performed, thereby forming the trench isolation TI directly above the image isolation region SPT. Subsequently, processes similar to those of the first embodiment shown in FIGS. 9 to 10 are performed, and then the subsequent steps of FIG. 10 are performed in a manner similar to that of the first embodiment, thereby forming the structure shown in FIG. 42 .
以下将说明本实施例的效果和优点。Effects and advantages of this embodiment will be described below.
深沟槽DT的非常高的纵横比例如可以避免沟槽如第九实施例那样仅被第三p型外延层PE3完全填充。如本实施例中那样提供涂覆了绝缘膜II以便以其填充沟槽空间的深沟槽DT。这使得其能够更完全地填充深沟槽DT以提高用于抑制电子串扰的像素隔离区SPT的效果。The very high aspect ratio of the deep trench DT can for example avoid that the trench is completely filled only by the third p-type epitaxial layer PE3 as in the ninth embodiment. The deep trench DT coated with the insulating film II so as to fill the trench space therewith is provided as in this embodiment. This makes it possible to more completely fill the deep trench DT to improve the effect of the pixel isolation region SPT for suppressing electronic crosstalk.
(第十一实施例)(eleventh embodiment)
参考图43,以下将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移晶体管TMI的构造。Referring to FIG. 43 , the configurations of the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described in detail below.
图43是示出与图4中所示的第一实施例相同的区域的模式的示意截面图。如图43所示,本实施例在具有主表面的p型衬底PSB1中,特别是在p型衬底PSB1的相对上部区域中具有掩埋层BRD(掩埋杂质层)。Fig. 43 is a schematic cross-sectional view showing a pattern of the same region as that of the first embodiment shown in Fig. 4 . As shown in FIG. 43, the present embodiment has a buried layer BRD (buried impurity layer) in the p-type substrate PSB1 having the main surface, particularly in the relatively upper region of the p-type substrate PSB1.
掩埋层BRD是包含多个扩展缺陷D2a的层,通过热处理引入半导体衬底PSB1中的诸如硼的p型杂质元素而获得扩展缺陷D2a。因此,从这点看,本实施例的掩埋层BRD具有例如类似于图27中所示的第四实施例的掩埋层BRD的构造和功能。The buried layer BRD is a layer containing a plurality of extended defects D2a obtained by heat-treating a p-type impurity element such as boron introduced into the semiconductor substrate PSB1. Therefore, from this point of view, the buried layer BRD of the present embodiment has, for example, a configuration and function similar to that of the buried layer BRD of the fourth embodiment shown in FIG. 27 .
上述掩埋层BRD的构造类似于图4中所示的第一实施例。具体来说,掩埋层BRD在其上具有第二p型外延层PE2(p型外延层),并且第二p型外延层PE2在其中具有包括光电二极管PD1的第一像素区RPx以及包括光电二极管PD2的第二像素区GPx。在第二像素区GPx中,第二p型外延层在其中具有第一注入区PJ1,因此覆盖掩埋层BRD的上表面。第一像素区RPx和第二像素区GPx在它们的边界部处具有第二注入区PJ2。The configuration of the above-mentioned buried layer BRD is similar to that of the first embodiment shown in FIG. 4 . Specifically, the buried layer BRD has thereon the second p-type epitaxial layer PE2 (p-type epitaxial layer), and the second p-type epitaxial layer PE2 has therein the first pixel region RPx including the photodiode PD1 and including the photodiode PD1. The second pixel area GPx of PD2. In the second pixel region GPx, the second p-type epitaxial layer has the first implantation region PJ1 therein, thus covering the upper surface of the buried layer BRD. The first pixel region RPx and the second pixel region GPx have a second injection region PJ2 at their boundary portions.
上述实施例在其半导体衬底SUB上都具有包括由硅制成的两个外延层,即第一p型外延层PE1和第二p型外延层PE2的构造。但是在本实施例中,形成在半导体衬底SUB上的外延层仅为一层,即第二p型外延层PE2。在本实施例中,在由硅制成的p型衬底PSB1中形成具有高于第二p型外延层的p型杂质浓度的掩埋层BRD,以替代第一p型外延层PE1。因此,类似于第一p型外延层PE1,其具有作为用于抑制p型衬底PSB1中产生的电子进入第二p型外延层PE2的势垒的功能。The above-described embodiments each have a configuration including two epitaxial layers made of silicon, ie, the first p-type epitaxial layer PE1 and the second p-type epitaxial layer PE2, on the semiconductor substrate SUB thereof. However, in this embodiment, only one epitaxial layer is formed on the semiconductor substrate SUB, that is, the second p-type epitaxial layer PE2. In this embodiment, a buried layer BRD having a p-type impurity concentration higher than that of the second p-type epitaxial layer is formed in a p-type substrate PSB1 made of silicon instead of the first p-type epitaxial layer PE1. Therefore, similarly to the first p-type epitaxial layer PE1, it has a function as a potential barrier for suppressing entry of electrons generated in the p-type substrate PSB1 into the second p-type epitaxial layer PE2.
如上所述,本实施例不同于具有第一类型外延层PE1的第一实施例之处在于在p型衬底PSB1中形成了掩埋层BRD。但是其具有基本上类似于第一实施例的构造,并且第一实施例的第一p型外延层PE1由掩埋层BRD替代。As described above, the present embodiment differs from the first embodiment having the first type epitaxial layer PE1 in that the buried layer BRD is formed in the p-type substrate PSB1. But it has a configuration basically similar to that of the first embodiment, and the first p-type epitaxial layer PE1 of the first embodiment is replaced by the buried layer BRD.
除上述要点之外,本实施例的构造基本上类似于图4中所示的第一实施例,因此相同的部件由相同参考数字表示,并且省略其重复说明。Except for the above points, the configuration of this embodiment is basically similar to that of the first embodiment shown in FIG. 4 , so the same components are denoted by the same reference numerals, and repeated description thereof is omitted.
参考图44和45,以下将详细说明构成作为本实施例的半导体器件的半导体成像器件的光电二极管PD以及包括光电二极管PD的转移晶体管TMI的构造。在图44和45中,示出类似于图43的区域的处理。Referring to FIGS. 44 and 45 , the configurations of the photodiode PD constituting the semiconductor imaging device as the semiconductor device of the present embodiment and the transfer transistor TMI including the photodiode PD will be described in detail below. In FIGS. 44 and 45 , processing of an area similar to that of FIG. 43 is shown.
如图44所示,类似于图5和6中所示的第一实施例,提供作为p型衬底的例如由硅制成并具有主表面S1的p型衬底PSB1。通过采用典型的离子注入技术将例如硼的杂质元素从p型衬底PSB1的上述主表面S1引入p型衬底PSB1中。随后,执行热处理以掩埋由此引入的诸如硼的杂质元素而作为诸如所谓的位错环的扩展缺陷S2a。富集由此引入的诸如硼的杂质的区域形成为掩埋层BRD。掩埋层BRD形成为具有高于将在下文说明的第二p型外延层PE2的p型杂质浓度。As shown in FIG. 44, similarly to the first embodiment shown in FIGS. 5 and 6, a p-type substrate PSB1 made of, for example, silicon and having a main surface S1 is provided as a p-type substrate. An impurity element such as boron is introduced into the p-type substrate PSB1 from the above-mentioned main surface S1 of the p-type substrate PSB1 by employing a typical ion implantation technique. Subsequently, heat treatment is performed to bury impurity elements such as boron thus introduced as extended defects S2a such as so-called dislocation loops. A region enriched with impurities such as boron thus introduced is formed as the buried layer BRD. The buried layer BRD is formed to have a p-type impurity concentration higher than that of the second p-type epitaxial layer PE2 which will be described below.
随后,在掩埋层BRD上形成由硅制成的第二p型外延层PE2。本实施例中的掩埋层BRD形成在p型衬底PSB1的相对上部中。掩埋层BRD的最上部和p型衬底PSB1的上侧上的主表面S1在它们之间包括具有等于典型的p型衬底PSB1的杂质浓度并且不具有BRD的区域。但是第二p型外延层PE2具有基本上等于p型衬底PSB1的p型杂质浓度,并且它们通用的,这是因为例如通过采用硼的杂质形成作为p型衬底的衬底。因此,p型衬底PSB1和第二p型外延层PE2之间的边界基本上消失,这意味着形成第二p型外延层PE2以便以其覆盖掩埋层BRD的上表面。Subsequently, a second p-type epitaxial layer PE2 made of silicon is formed on the buried layer BRD. The buried layer BRD in this embodiment is formed in the relatively upper portion of the p-type substrate PSB1. The uppermost part of the buried layer BRD and the main surface S1 on the upper side of the p-type substrate PSB1 include therebetween a region having an impurity concentration equal to that of a typical p-type substrate PSB1 and having no BRD. But the second p-type epitaxial layer PE2 has a p-type impurity concentration substantially equal to that of the p-type substrate PSB1, and they are common because the substrate as a p-type substrate is formed by using an impurity of boron, for example. Therefore, the boundary between the p-type substrate PSB1 and the second p-type epitaxial layer PE2 substantially disappears, which means that the second p-type epitaxial layer PE2 is formed so as to cover the upper surface of the buried layer BRD therewith.
如图45所示,类似于图8至10中所示的第一实施例,光电二极管PD1等形成在第二p型外延层PE2中,随后执行类似于图10中所示的第一实施例的后续步骤以获得图43中所示的结构。As shown in FIG. 45, similarly to the first embodiment shown in FIGS. Subsequent steps to obtain the structure shown in Figure 43.
以下将说明本实施例的效果和优点。Effects and advantages of this embodiment will be described below.
在本实施例中,仅第二p型外延层PE2形成为p型外延层,并且利用离子注入技术形成掩埋层BRD,从而替代另一实施例中的第一p型外延层PE1。相比于采用外延生长形成势垒,通过采用离子注入技术形成的势垒可以降低成本。In this embodiment, only the second p-type epitaxial layer PE2 is formed as a p-type epitaxial layer, and the buried layer BRD is formed by ion implantation technology, thereby replacing the first p-type epitaxial layer PE1 in another embodiment. Compared with the barrier formed by epitaxial growth, the barrier formed by ion implantation technology can reduce the cost.
最后,将说明一个实施例的要点。Finally, the gist of an embodiment will be explained.
如图46所示,一个实施例的半导体器件包括具有主表面的半导体衬底SUB1,形成在主表面上的第一p型外延层PE1,形成为覆盖第一外延层PE1的上表面的第二p型外延层PE2,以及形成在第二p型外延层PE2中的第一光电转换元件PD1。第一和第二p型外延层PE1和PE2每个都由硅制成。第一p型外延层PE1具有高于第二p型外延层PE2的p型杂质浓度。除上述要点外,图46中所示的构造类似于图4中所示的构造。As shown in FIG. 46, a semiconductor device according to an embodiment includes a semiconductor substrate SUB1 having a main surface, a first p-type epitaxial layer PE1 formed on the main surface, and a second p-type epitaxial layer PE1 formed to cover the upper surface of the first epitaxial layer PE1. The p-type epitaxial layer PE2, and the first photoelectric conversion element PD1 formed in the second p-type epitaxial layer PE2. Each of the first and second p-type epitaxial layers PE1 and PE2 is made of silicon. The first p-type epitaxial layer PE1 has a higher p-type impurity concentration than the second p-type epitaxial layer PE2. The configuration shown in FIG. 46 is similar to the configuration shown in FIG. 4 except for the above points.
虽然会与上述说明书重复,但是以下将说明实施例中说明的某些细节。While repeating the description above, some of the details illustrated in the Examples will be described below.
(1)制造半导体器件的方法开始于提供具有主表面的半导体衬底。第一p型外延层形成在主表面上。第二p型外延层形成为以其覆盖第一p型外延层的上表面。第一光电转换元件形成在第二p型外延层中。第一和第二p型外延层每个都由硅制成,并且第一p型外延层具有高于第二p型外延层的类型的杂质浓度。(1) A method of manufacturing a semiconductor device starts with providing a semiconductor substrate having a main surface. A first p-type epitaxial layer is formed on the main surface. The second p-type epitaxial layer is formed such that it covers the upper surface of the first p-type epitaxial layer. The first photoelectric conversion element is formed in the second p-type epitaxial layer. Each of the first and second p-type epitaxial layers is made of silicon, and the first p-type epitaxial layer has an impurity concentration of a type higher than that of the second p-type epitaxial layer.
(2)在(1)中说明的制造半导体器件的方法中,半导体衬底是p型衬底,并且半导体衬底的缺陷密度高于第二p型外延层的缺陷密度。(2) In the method of manufacturing a semiconductor device described in (1), the semiconductor substrate is a p-type substrate, and the defect density of the semiconductor substrate is higher than that of the second p-type epitaxial layer.
(3)在(1)中说明的制造半导体器件的方法,半导体衬底是p型衬底。在提供半导体衬底时,进一步在半导体衬底中形成扩展缺陷。在半导体衬底中形成扩展缺陷时,将p型杂质引入半导体衬底中,使得半导体衬底中的p型杂质浓度变得高于第二p型外延层中的p型杂质浓度。通过热处理最终形成的半导体衬底以致使半导体衬底中的p型杂质和扩散进入半导体衬底的氧之间的反应,第一扩展缺陷形成为扩展缺陷。(3) In the method of manufacturing a semiconductor device described in (1), the semiconductor substrate is a p-type substrate. When the semiconductor substrate is provided, extended defects are further formed in the semiconductor substrate. When the extended defect is formed in the semiconductor substrate, p-type impurities are introduced into the semiconductor substrate so that the p-type impurity concentration in the semiconductor substrate becomes higher than the p-type impurity concentration in the second p-type epitaxial layer. The first extended defect is formed as an extended defect by heat-treating the finally formed semiconductor substrate to cause a reaction between p-type impurities in the semiconductor substrate and oxygen diffused into the semiconductor substrate.
(4)在(1)中说明的制造半导体器件的方法中,在提供半导体衬底时进一步在半导体衬底中形成扩展缺陷。在半导体衬底中形成扩展缺陷时,将杂质元素引入半导体衬底中。通过热处理具有其中引入了杂质元素的半导体衬底,第二扩展缺陷形成为扩展缺陷。(4) In the method of manufacturing a semiconductor device described in (1), extended defects are further formed in the semiconductor substrate when the semiconductor substrate is provided. When an extended defect is formed in a semiconductor substrate, an impurity element is introduced into the semiconductor substrate. The second extended defect is formed as an extended defect by heat-treating the semiconductor substrate having the impurity element introduced therein.
(5)在(1)中说明的制造半导体器件的方法中,第一p型外延层形成在主表面上,以便第一p型外延层包括多个层。在主表面上形成第一p型外延层时,由于衬底相邻层中的p型杂质和从半导体衬底扩散进入衬底相邻层中的氧之间的反应,因此第一扩展缺陷形成为衬底相邻层中的扩展缺陷,衬底相邻层是构成第一p型外延层的层之一并位于最接近半导体衬底的一侧上的层。(5) In the method of manufacturing a semiconductor device described in (1), the first p-type epitaxial layer is formed on the main surface so that the first p-type epitaxial layer includes a plurality of layers. When the first p-type epitaxial layer is formed on the main surface, due to the reaction between p-type impurities in the substrate-adjacent layer and oxygen diffused from the semiconductor substrate into the substrate-adjacent layer, the first extended defect forms is an extended defect in a substrate-adjacent layer, which is one of the layers constituting the first p-type epitaxial layer and located on the side closest to the semiconductor substrate.
(6)在(5)中说明的制造半导体器件的方法中,在主表面上形成第一p型外延层时,将构成第一p型外延层的多个层之中的、衬底相邻层中的氧浓度设定为高于除衬底相邻层之外的、构成第一p型外延层的多个层中的氧浓度。(6) In the method of manufacturing a semiconductor device described in (5), when the first p-type epitaxial layer is formed on the main surface, among the plurality of layers constituting the first p-type epitaxial layer, the substrates are adjacent to each other. The oxygen concentration in the layer is set to be higher than the oxygen concentration in layers constituting the first p-type epitaxial layer other than the substrate-adjacent layer.
(7)制造半导体器件的方法开始于具有主表面的半导体衬底的提供。杂质注入半导体衬底以形成掩埋杂质层。p型外延层形成在掩埋杂质层上。第一光电转换元件形成在p型外延层中。掩埋杂质层和p型外延层每个都由硅制成,并且掩埋杂质层具有高于p型外延层的p型杂质浓度。(7) A method of manufacturing a semiconductor device starts with the provision of a semiconductor substrate having a main surface. Impurities are implanted into the semiconductor substrate to form buried impurity layers. A p-type epitaxial layer is formed on the buried impurity layer. The first photoelectric conversion element is formed in the p-type epitaxial layer. The buried impurity layer and the p-type epitaxial layer are each made of silicon, and the buried impurity layer has a higher p-type impurity concentration than the p-type epitaxial layer.
已经基于某些实施例具体说明了由本发明人提出的本发明。毋容质疑的是本发明不限于这些实施例或由这些实施例局限,而是可在不脱离本发明范围的情况下进行各种改变。The invention made by the present inventors has been specifically described based on certain embodiments. It is needless to say that the present invention is not limited to or by these embodiments, but various changes can be made without departing from the scope of the present invention.
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Also Published As
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US9437644B2 (en) | 2016-09-06 |
JP2015095484A (en) | 2015-05-18 |
JP6302216B2 (en) | 2018-03-28 |
US20150130009A1 (en) | 2015-05-14 |
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